Qiskit – Quantum Computing Framework

Open-source quantum computing framework for building, simulating, and running quantum algorithms on quantum computers and simulators.

When to Use

• Building quantum circuits and gates
• Running quantum algorithms (VQE, QAOA, Grover, Shor)
• Quantum chemistry calculations (integration with PySCF)
• Quantum machine learning
• Quantum simulation and noise modeling
• Transpiling circuits for real quantum hardware
• Quantum optimization problems
• Quantum error correction
• Quantum cryptography
• Educational quantum computing demonstrations

Reference Documentation

Official docs: https://qiskit.org/documentation/
Search patterns: qiskit.circuit.QuantumCircuit, qiskit.algorithms.VQE, qiskit.quantum_info, qiskit_nature

Core Principles

Use Qiskit For

Do NOT Use For

• Classical machine learning (use scikit-learn, PyTorch)
• Classical optimization (use SciPy)
• General numerical computing (use NumPy)
• Classical cryptography (use cryptography package)
• Large-scale classical simulation (use classical simulators)

Quick Reference

Installation

# Core Qiskit
pip install qiskit

# With visualization tools
pip install qiskit[visualization]

# Quantum chemistry extension
pip install qiskit-nature qiskit-nature-pyscf

# Machine learning extension
pip install qiskit-machine-learning

# Optimization extension
pip install qiskit-optimization

# Full installation
pip install 'qiskit[all]' qiskit-nature qiskit-machine-learning qiskit-optimization

Standard Imports

# Core imports
from qiskit import QuantumCircuit, QuantumRegister, ClassicalRegister
from qiskit import transpile, assemble
from qiskit.providers.aer import AerSimulator
from qiskit.visualization import plot_histogram, plot_bloch_multivector

# Quantum algorithms
from qiskit.algorithms import VQE, QAOA, Grover, Shor
from qiskit.algorithms.optimizers import SLSQP, COBYLA, SPSA

# Quantum info
from qiskit.quantum_info import Statevector, DensityMatrix, Operator
from qiskit.quantum_info import entropy, entanglement_of_formation

# Circuit library
from qiskit.circuit.library import QFT, RealAmplitudes, EfficientSU2

Basic Pattern – Circuit Building

from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator

# Create circuit
qc = QuantumCircuit(2, 2)

# Add gates
qc.h(0)              # Hadamard on qubit 0
qc.cx(0, 1)          # CNOT from 0 to 1

# Measure
qc.measure([0, 1], [0, 1])

# Simulate
simulator = AerSimulator()
job = simulator.run(qc, shots=1000)
result = job.result()
counts = result.get_counts()

print(f"Results: {counts}")

Basic Pattern – Quantum Algorithm

from qiskit import QuantumCircuit
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.circuit.library import RealAmplitudes
from qiskit.primitives import Estimator
from qiskit.quantum_info import SparsePauliOp

# Define Hamiltonian
hamiltonian = SparsePauliOp(['ZZ', 'IZ', 'ZI'], coeffs=[1.0, -0.5, -0.5])

# Create ansatz
ansatz = RealAmplitudes(num_qubits=2, reps=1)

# Setup VQE
optimizer = SLSQP(maxiter=100)
estimator = Estimator()
vqe = VQE(estimator, ansatz, optimizer)

# Run
result = vqe.compute_minimum_eigenvalue(hamiltonian)
print(f"Ground state energy: {result.eigenvalue:.6f}")

Critical Rules

✅ DO

• Use simulators for development – Test on simulators before real hardware
• Transpile for target backend – Always transpile circuits for specific hardware
• Handle measurement statistics – Work with shot counts, not single results
• Use primitives for algorithms – Use Estimator/Sampler primitives
• Check circuit depth – Monitor gate count and depth for real hardware
• Implement error mitigation – Use error mitigation for noisy hardware
• Validate quantum states – Check state validity and normalization
• Use appropriate basis gates – Match hardware native gates
• Set random seed for reproducibility – Use seed for consistent results
• Monitor job status – Check if quantum jobs complete successfully

❌ DON’T

• Ignore hardware constraints – Real quantum computers have limitations
• Use too many qubits on simulators – Memory grows exponentially
• Forget to measure – Quantum states collapse on measurement
• Mix classical and quantum incorrectly – Understand measurement timing
• Ignore decoherence – Quantum states decay over time
• Over-transpile – Unnecessary transpilation adds gates
• Assume perfect gates – Real gates have errors
• Ignore topology – Not all qubits are connected
• Use deprecated APIs – Qiskit evolves rapidly
• Run without error handling – Quantum jobs can fail

Anti-Patterns (NEVER)

from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator
from qiskit.primitives import Estimator

# ❌ BAD: No measurement
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
# Forgot qc.measure()!

# ✅ GOOD: Always measure when needed
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])

# ❌ BAD: Using deprecated execute()
from qiskit import execute
result = execute(qc, backend, shots=1024).result()

# ✅ GOOD: Use new run() method
simulator = AerSimulator()
job = simulator.run(qc, shots=1024)
result = job.result()

# ❌ BAD: Assuming perfect measurement
counts = result.get_counts()
# Assuming exactly 50/50 split!
assert counts['00'] == 512

# ✅ GOOD: Handle statistical variation
counts = result.get_counts()
ratio = counts.get('00', 0) / sum(counts.values())
print(f"Measured |00⟩ with probability {ratio:.3f}")

# ❌ BAD: Not checking circuit properties
qc = QuantumCircuit(20)  # Many qubits!
# Adding many gates...
# Trying to simulate without checking depth/size!

# ✅ GOOD: Check circuit properties
qc = QuantumCircuit(20)
# ... add gates ...
print(f"Circuit depth: {qc.depth()}")
print(f"Gate count: {len(qc.data)}")
print(f"Qubits: {qc.num_qubits}")

# ❌ BAD: Ignoring transpilation
job = backend.run(qc)  # May fail on real hardware!

# ✅ GOOD: Transpile for backend
from qiskit import transpile
transpiled_qc = transpile(qc, backend=backend, optimization_level=3)
job = backend.run(transpiled_qc)

Quantum Circuits (qiskit.QuantumCircuit)

Basic Circuit Construction

from qiskit import QuantumCircuit, QuantumRegister, ClassicalRegister
import numpy as np

# Method 1: Simple initialization
qc = QuantumCircuit(3, 3)  # 3 qubits, 3 classical bits

# Method 2: Using registers
qr = QuantumRegister(3, 'q')
cr = ClassicalRegister(3, 'c')
qc = QuantumCircuit(qr, cr)

# Method 3: Multiple registers
qr1 = QuantumRegister(2, 'data')
qr2 = QuantumRegister(1, 'ancilla')
cr = ClassicalRegister(2, 'meas')
qc = QuantumCircuit(qr1, qr2, cr)

print(f"Number of qubits: {qc.num_qubits}")
print(f"Number of classical bits: {qc.num_clbits}")
print(f"Circuit depth: {qc.depth()}")

Single-Qubit Gates

from qiskit import QuantumCircuit
import numpy as np

qc = QuantumCircuit(1)

# Pauli gates
qc.x(0)   # Pauli X (NOT gate)
qc.y(0)   # Pauli Y
qc.z(0)   # Pauli Z

# Hadamard gate
qc.h(0)   # Creates superposition

# Phase gates
qc.s(0)   # S gate (π/2 phase)
qc.t(0)   # T gate (π/4 phase)
qc.sdg(0) # S dagger
qc.tdg(0) # T dagger

# Rotation gates
qc.rx(np.pi/4, 0)  # Rotation around X
qc.ry(np.pi/4, 0)  # Rotation around Y
qc.rz(np.pi/4, 0)  # Rotation around Z

# General rotation
qc.u(np.pi/4, np.pi/2, np.pi, 0)  # U gate

# Identity (wait)
qc.id(0)

print(f"Gate count: {len(qc.data)}")

Two-Qubit Gates

from qiskit import QuantumCircuit
import numpy as np

qc = QuantumCircuit(2)

# CNOT (Controlled-NOT)
qc.cx(0, 1)  # Control: 0, Target: 1

# Other controlled gates
qc.cy(0, 1)  # Controlled-Y
qc.cz(0, 1)  # Controlled-Z
qc.ch(0, 1)  # Controlled-Hadamard

# SWAP gate
qc.swap(0, 1)

# Controlled phase
qc.cp(np.pi/4, 0, 1)

# Controlled-U
qc.cu(np.pi/4, np.pi/2, np.pi, 0, 0, 1)

# Toffoli (CCX) - needs 3 qubits
qc_3 = QuantumCircuit(3)
qc_3.ccx(0, 1, 2)  # Controls: 0,1, Target: 2

print(qc.draw())

Creating Entanglement

from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator
from qiskit.quantum_info import Statevector

# Bell state (maximally entangled)
def create_bell_state():
    qc = QuantumCircuit(2)
    qc.h(0)
    qc.cx(0, 1)
    return qc

bell = create_bell_state()
state = Statevector.from_instruction(bell)
print(f"Bell state: {state}")

# GHZ state (3-qubit entanglement)
def create_ghz_state(n):
    qc = QuantumCircuit(n)
    qc.h(0)
    for i in range(n-1):
        qc.cx(i, i+1)
    return qc

ghz = create_ghz_state(3)
state_ghz = Statevector.from_instruction(ghz)
print(f"GHZ state: {state_ghz}")

# W state (another type of 3-qubit entanglement)
def create_w_state():
    qc = QuantumCircuit(3)
    qc.ry(1.9106, 0)
    qc.ch(0, 1)
    qc.x(0)
    qc.cy(0, 1)
    qc.ccx(0, 1, 2)
    qc.x(0)
    return qc

w = create_w_state()
print(f"W state circuit depth: {w.depth()}")

Parameterized Circuits

from qiskit import QuantumCircuit
from qiskit.circuit import Parameter, ParameterVector
import numpy as np

# Single parameter
theta = Parameter('θ')
qc = QuantumCircuit(1)
qc.ry(theta, 0)

# Bind parameter
bound_qc = qc.bind_parameters({theta: np.pi/4})
print(f"Unbound: {qc}")
print(f"Bound: {bound_qc}")

# Multiple parameters
params = ParameterVector('θ', 4)
qc_param = QuantumCircuit(2)
qc_param.ry(params[0], 0)
qc_param.ry(params[1], 1)
qc_param.cx(0, 1)
qc_param.ry(params[2], 0)
qc_param.ry(params[3], 1)

# Bind all parameters
values = [np.pi/4, np.pi/3, np.pi/2, np.pi/6]
bound = qc_param.bind_parameters(dict(zip(params, values)))

print(f"Number of parameters: {qc_param.num_parameters}")

Quantum Algorithms

Variational Quantum Eigensolver (VQE)

from qiskit import QuantumCircuit
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP, COBYLA
from qiskit.circuit.library import RealAmplitudes, EfficientSU2
from qiskit.primitives import Estimator
from qiskit.quantum_info import SparsePauliOp
import numpy as np

# Define Hamiltonian (e.g., H2 molecule)
# H = -1.05 * ZZ + 0.39 * XX - 0.39 * YY - 0.01 * ZI
hamiltonian = SparsePauliOp(
    ['ZZ', 'XX', 'YY', 'ZI', 'IZ'],
    coeffs=[-1.05, 0.39, -0.39, -0.01, -0.01]
)

# Create ansatz (variational form)
ansatz = RealAmplitudes(num_qubits=2, reps=2)

# Alternative: EfficientSU2
# ansatz = EfficientSU2(num_qubits=2, reps=2)

# Setup optimizer
optimizer = SLSQP(maxiter=100)

# Create estimator primitive
estimator = Estimator()

# Setup and run VQE
vqe = VQE(estimator, ansatz, optimizer)
result = vqe.compute_minimum_eigenvalue(hamiltonian)

print(f"Ground state energy: {result.eigenvalue:.6f}")
print(f"Optimal parameters: {result.optimal_parameters}")
print(f"Optimizer evaluations: {result.cost_function_evals}")

# Get optimal circuit
optimal_circuit = ansatz.bind_parameters(result.optimal_point)
print(f"\nOptimal circuit depth: {optimal_circuit.depth()}")

QAOA (Quantum Approximate Optimization Algorithm)

from qiskit import QuantumCircuit
from qiskit.algorithms import QAOA
from qiskit.algorithms.optimizers import COBYLA
from qiskit.primitives import Sampler
from qiskit.quantum_info import SparsePauliOp
import numpy as np

# Max-Cut problem on a triangle graph
# Cost Hamiltonian: H = (1-Z0*Z1)/2 + (1-Z1*Z2)/2 + (1-Z0*Z2)/2
cost_hamiltonian = SparsePauliOp(
    ['ZZ', 'ZI', 'IZ'],
    coeffs=[0.5, -0.5, -0.5]
)

# Setup QAOA
optimizer = COBYLA(maxiter=100)
sampler = Sampler()
qaoa = QAOA(sampler, optimizer, reps=2)

# Run QAOA
result = qaoa.compute_minimum_eigenvalue(cost_hamiltonian)

print(f"Optimal objective: {result.eigenvalue:.6f}")
print(f"Optimal parameters: {result.optimal_parameters}")

# Most probable solution
from qiskit.result import QuasiDistribution
prob_dist = result.eigenstate
if isinstance(prob_dist, QuasiDistribution):
    most_likely = max(prob_dist, key=prob_dist.get)
    print(f"Most likely solution: {bin(most_likely)[2:].zfill(2)}")

Grover’s Algorithm (Quantum Search)

from qiskit import QuantumCircuit
from qiskit.algorithms import Grover, AmplificationProblem
from qiskit.circuit.library import GroverOperator
from qiskit.primitives import Sampler
import numpy as np

def grover_search(marked_states, n_qubits):
    """
    Grover's algorithm to find marked states.
    
    Args:
        marked_states: List of marked states (e.g., ['101', '110'])
        n_qubits: Number of qubits
    """
    # Create oracle that marks the target states
    oracle = QuantumCircuit(n_qubits)
    
    # Mark state |101⟩ by flipping phase
    if '101' in marked_states:
        oracle.x([0, 2])  # Flip to make 101 -> 111
        oracle.h(2)
        oracle.ccx(0, 1, 2)
        oracle.h(2)
        oracle.x([0, 2])  # Flip back
    
    # Grover diffusion operator
    diffusion = QuantumCircuit(n_qubits)
    diffusion.h(range(n_qubits))
    diffusion.x(range(n_qubits))
    diffusion.h(n_qubits - 1)
    diffusion.mcx(list(range(n_qubits - 1)), n_qubits - 1)
    diffusion.h(n_qubits - 1)
    diffusion.x(range(n_qubits))
    diffusion.h(range(n_qubits))
    
    # Complete Grover iteration
    grover_op = oracle.compose(diffusion)
    
    # Setup and run
    problem = AmplificationProblem(oracle, is_good_state=marked_states)
    grover = Grover(sampler=Sampler())
    result = grover.amplify(problem)
    
    return result

# Example: Search for |101⟩ in 3-qubit space
result = grover_search(['101'], 3)
print(f"Top measurement: {result.top_measurement}")
print(f"Oracle evaluations: {result.oracle_evaluation}")

# Simpler example: 2-qubit search
qc = QuantumCircuit(2, 2)
qc.h([0, 1])  # Superposition

# Oracle marks |11⟩
qc.cz(0, 1)

# Diffusion
qc.h([0, 1])
qc.x([0, 1])
qc.cz(0, 1)
qc.x([0, 1])
qc.h([0, 1])

qc.measure([0, 1], [0, 1])

from qiskit.providers.aer import AerSimulator
simulator = AerSimulator()
job = simulator.run(qc, shots=1000)
counts = job.result().get_counts()
print(f"Grover results: {counts}")

Quantum Phase Estimation (QPE)

from qiskit import QuantumCircuit
from qiskit.circuit.library import QFT
from qiskit.providers.aer import AerSimulator
import numpy as np

def quantum_phase_estimation(unitary, n_counting_qubits):
    """
    Estimate the phase of an eigenstate of a unitary operator.
    
    Args:
        unitary: Unitary operator as a QuantumCircuit
        n_counting_qubits: Precision qubits
    """
    n_system_qubits = unitary.num_qubits
    
    qc = QuantumCircuit(n_counting_qubits + n_system_qubits, n_counting_qubits)
    
    # Initialize eigenstate (simplified: use |1⟩)
    qc.x(n_counting_qubits)
    
    # Hadamard on counting qubits
    for i in range(n_counting_qubits):
        qc.h(i)
    
    # Controlled-U^(2^i) operations
    repetitions = 1
    for counting_qubit in range(n_counting_qubits):
        for _ in range(repetitions):
            qc.append(unitary.control(), [counting_qubit] + 
                     list(range(n_counting_qubits, n_counting_qubits + n_system_qubits)))
        repetitions *= 2
    
    # Inverse QFT
    qc.append(QFT(n_counting_qubits, inverse=True), range(n_counting_qubits))
    
    # Measure counting qubits
    qc.measure(range(n_counting_qubits), range(n_counting_qubits))
    
    return qc

# Example: Phase estimation for T gate (phase π/4)
t_gate = QuantumCircuit(1)
t_gate.t(0)

qpe_circuit = quantum_phase_estimation(t_gate, n_counting_qubits=3)

simulator = AerSimulator()
job = simulator.run(qpe_circuit, shots=1000)
counts = job.result().get_counts()
print(f"Phase estimation results: {counts}")

# Most common result gives phase
most_common = max(counts, key=counts.get)
phase_estimate = int(most_common, 2) / (2**3)
print(f"Estimated phase: {phase_estimate * 2 * np.pi:.4f} rad")
print(f"True phase: {np.pi/4:.4f} rad")

Quantum Chemistry with Qiskit Nature

Molecular Ground State Calculation

# Requires: pip install qiskit-nature qiskit-nature-pyscf

from qiskit_nature.units import DistanceUnit
from qiskit_nature.second_q.drivers import PySCFDriver
from qiskit_nature.second_q.mappers import JordanWignerMapper, ParityMapper
from qiskit_nature.second_q.circuit.library import HartreeFock, UCCSD
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.primitives import Estimator
import numpy as np

# Define molecule (H2)
driver = PySCFDriver(
    atom='H 0 0 0; H 0 0 0.735',
    basis='sto3g',
    charge=0,
    spin=0,
    unit=DistanceUnit.ANGSTROM
)

# Get problem
problem = driver.run()
hamiltonian = problem.hamiltonian.second_q_op()

# Map to qubits
mapper = JordanWignerMapper()
qubit_op = mapper.map(hamiltonian)

print(f"Number of qubits required: {qubit_op.num_qubits}")

# Initial state (Hartree-Fock)
num_particles = problem.num_particles
num_spatial_orbitals = problem.num_spatial_orbitals

init_state = HartreeFock(
    num_spatial_orbitals=num_spatial_orbitals,
    num_particles=num_particles,
    qubit_mapper=mapper
)

# Ansatz (UCCSD)
ansatz = UCCSD(
    num_spatial_orbitals=num_spatial_orbitals,
    num_particles=num_particles,
    qubit_mapper=mapper,
    initial_state=init_state
)

# VQE calculation
optimizer = SLSQP(maxiter=100)
estimator = Estimator()

vqe = VQE(estimator, ansatz, optimizer)
result = vqe.compute_minimum_eigenvalue(qubit_op)

print(f"\nVQE Ground State Energy: {result.eigenvalue:.6f} Ha")
print(f"Reference HF energy: {problem.reference_energy:.6f} Ha")

Excited States Calculation

from qiskit_nature.second_q.algorithms import GroundStateEigensolver, ExcitedStatesEigensolver
from qiskit_nature.second_q.algorithms import QEOM
from qiskit_nature.second_q.mappers import JordanWignerMapper
from qiskit_nature.second_q.drivers import PySCFDriver
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.primitives import Estimator

# Setup molecule
driver = PySCFDriver(atom='H 0 0 0; H 0 0 0.735', basis='sto3g')
problem = driver.run()

# Mapper
mapper = JordanWignerMapper()

# Ground state solver
optimizer = SLSQP(maxiter=100)
estimator = Estimator()

# Simple ansatz for demonstration
from qiskit.circuit.library import RealAmplitudes
ansatz = RealAmplitudes(num_qubits=4, reps=2)

vqe = VQE(estimator, ansatz, optimizer)
ground_solver = GroundStateEigensolver(mapper, vqe)

# Calculate ground state
ground_result = ground_solver.solve(problem)
print(f"Ground state energy: {ground_result.total_energies[0]:.6f} Ha")

# Excited states with QEOM
qeom = QEOM(ground_solver, 'sd')  # singles and doubles
excited_solver = ExcitedStatesEigensolver(mapper, qeom)

# Calculate excited states
excited_result = excited_solver.solve(problem)
print(f"\nExcited state energies:")
for i, energy in enumerate(excited_result.total_energies):
    print(f"State {i}: {energy:.6f} Ha")

Molecular Potential Energy Surface

from qiskit_nature.second_q.drivers import PySCFDriver
from qiskit_nature.second_q.mappers import JordanWignerMapper
from qiskit_nature.second_q.algorithms import GroundStateEigensolver
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.primitives import Estimator
from qiskit.circuit.library import RealAmplitudes
import numpy as np

def calculate_pes(distances, molecule_template, basis='sto3g'):
    """
    Calculate potential energy surface for a diatomic molecule.
    
    Args:
        distances: Array of interatomic distances
        molecule_template: Molecule string with {} for distance
        basis: Basis set
    """
    energies = []
    
    for distance in distances:
        # Setup molecule at this distance
        atom_string = molecule_template.format(distance)
        driver = PySCFDriver(atom=atom_string, basis=basis)
        problem = driver.run()
        
        # Map to qubits
        mapper = JordanWignerMapper()
        
        # Simple VQE calculation
        ansatz = RealAmplitudes(num_qubits=4, reps=1)
        optimizer = SLSQP(maxiter=50)
        estimator = Estimator()
        
        vqe = VQE(estimator, ansatz, optimizer)
        solver = GroundStateEigensolver(mapper, vqe)
        
        # Calculate energy
        result = solver.solve(problem)
        energies.append(result.total_energies[0])
        
        print(f"Distance {distance:.2f} Å: Energy = {energies[-1]:.6f} Ha")
    
    return np.array(energies)

# Calculate PES for H2
distances = np.linspace(0.5, 2.5, 5)  # Angstroms
molecule_template = 'H 0 0 0; H 0 0 {}'

energies = calculate_pes(distances, molecule_template)

# Find equilibrium bond length
min_idx = np.argmin(energies)
print(f"\nEquilibrium bond length: {distances[min_idx]:.2f} Å")
print(f"Minimum energy: {energies[min_idx]:.6f} Ha")

Quantum Simulation

Hamiltonian Simulation with Trotter

from qiskit import QuantumCircuit
from qiskit.quantum_info import SparsePauliOp, Statevector
from qiskit.synthesis import SuzukiTrotter
import numpy as np

def trotter_simulation(hamiltonian, time, n_steps):
    """
    Simulate time evolution under Hamiltonian using Trotter decomposition.
    
    Args:
        hamiltonian: SparsePauliOp Hamiltonian
        time: Total evolution time
        n_steps: Number of Trotter steps
    """
    dt = time / n_steps
    
    # Create Trotter circuit
    n_qubits = hamiltonian.num_qubits
    qc = QuantumCircuit(n_qubits)
    
    # Initial state (e.g., |0⟩)
    # Apply Trotter steps
    for _ in range(n_steps):
        # For each Pauli term in Hamiltonian
        for pauli, coeff in zip(hamiltonian.paulis, hamiltonian.coeffs):
            # Apply exp(-i * coeff * dt * pauli)
            angle = 2 * float(coeff.real) * dt
            
            # Simple implementation for single Pauli terms
            pauli_str = str(pauli)
            
            # Apply appropriate rotation
            if 'Z' in pauli_str and pauli_str.count('I') == n_qubits - 1:
                idx = pauli_str.index('Z')
                qc.rz(angle, n_qubits - 1 - idx)
            elif 'X' in pauli_str and pauli_str.count('I') == n_qubits - 1:
                idx = pauli_str.index('X')
                qc.rx(angle, n_qubits - 1 - idx)
    
    return qc

# Example: Ising model Hamiltonian
hamiltonian = SparsePauliOp(['ZZ', 'XI', 'IX'], coeffs=[1.0, -0.5, -0.5])

# Simulate for time t=1.0 with 10 Trotter steps
qc = trotter_simulation(hamiltonian, time=1.0, n_steps=10)

print(f"Trotter circuit depth: {qc.depth()}")
print(f"Gate count: {len(qc.data)}")

# Get final state
state = Statevector.from_instruction(qc)
print(f"Final state vector: {state[:4]}")  # First 4 amplitudes

Variational Quantum Simulation

from qiskit import QuantumCircuit
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.circuit.library import RealAmplitudes
from qiskit.primitives import Estimator
from qiskit.quantum_info import SparsePauliOp
import numpy as np

def simulate_dynamics(hamiltonian, initial_state_circuit, times, ansatz_reps=2):
    """
    Simulate quantum dynamics using VQE at different times.
    
    Args:
        hamiltonian: Time-evolution Hamiltonian
        initial_state_circuit: Circuit preparing initial state
        times: Array of times to simulate
        ansatz_reps: Repetitions in ansatz
    """
    n_qubits = hamiltonian.num_qubits
    results = []
    
    for t in times:
        # Time-evolved Hamiltonian: H(t) = exp(-iHt) ρ(0) exp(iHt)
        # Approximate with VQE
        
        ansatz = RealAmplitudes(num_qubits=n_qubits, reps=ansatz_reps)
        
        # Combine initial state + ansatz
        full_circuit = initial_state_circuit.copy()
        full_circuit.compose(ansatz, inplace=True)
        
        optimizer = SLSQP(maxiter=100)
        estimator = Estimator()
        
        vqe = VQE(estimator, full_circuit, optimizer)
        result = vqe.compute_minimum_eigenvalue(hamiltonian)
        
        results.append({
            'time': t,
            'energy': result.eigenvalue,
            'parameters': result.optimal_parameters
        })
        
        print(f"Time {t:.2f}: Energy = {result.eigenvalue:.6f}")
    
    return results

# Example: Simulate Heisenberg model
hamiltonian = SparsePauliOp(
    ['XX', 'YY', 'ZZ'],
    coeffs=[0.5, 0.5, 0.5]
)

# Initial state: |01⟩
initial_state = QuantumCircuit(2)
initial_state.x(1)

# Simulate at different times
times = np.linspace(0, 2, 5)
results = simulate_dynamics(hamiltonian, initial_state, times)

Quantum Machine Learning

Quantum Kernel Method

# Requires: pip install qiskit-machine-learning

from qiskit_machine_learning.kernels import FidelityQuantumKernel
from qiskit.circuit.library import ZZFeatureMap
from qiskit.primitives import Sampler
from sklearn.svm import SVC
import numpy as np

# Generate synthetic data
np.random.seed(42)
X_train = np.random.rand(20, 2) * 2 * np.pi
y_train = (X_train[:, 0] + X_train[:, 1] > np.pi).astype(int)

X_test = np.random.rand(10, 2) * 2 * np.pi
y_test = (X_test[:, 0] + X_test[:, 1] > np.pi).astype(int)

# Create feature map
feature_map = ZZFeatureMap(feature_dimension=2, reps=2)

# Create quantum kernel
sampler = Sampler()
quantum_kernel = FidelityQuantumKernel(feature_map=feature_map, fidelity=sampler)

# Compute kernel matrix
kernel_matrix_train = quantum_kernel.evaluate(x_vec=X_train)
kernel_matrix_test = quantum_kernel.evaluate(x_vec=X_test, y_vec=X_train)

print(f"Training kernel matrix shape: {kernel_matrix_train.shape}")
print(f"Test kernel matrix shape: {kernel_matrix_test.shape}")

# Use with SVM
svc = SVC(kernel='precomputed')
svc.fit(kernel_matrix_train, y_train)

# Predict
predictions = svc.predict(kernel_matrix_test)
accuracy = np.mean(predictions == y_test)

print(f"\nQuantum Kernel SVM Accuracy: {accuracy:.2%}")

Variational Quantum Classifier (VQC)

from qiskit_machine_learning.algorithms import VQC
from qiskit.circuit.library import RealAmplitudes, ZZFeatureMap
from qiskit.algorithms.optimizers import COBYLA
from qiskit.primitives import Sampler
import numpy as np

# Generate training data
np.random.seed(42)
X_train = np.random.rand(40, 2) * 2 - 1  # [-1, 1]
y_train = (X_train[:, 0]**2 + X_train[:, 1]**2 < 0.5).astype(int)

X_test = np.random.rand(20, 2) * 2 - 1
y_test = (X_test[:, 0]**2 + X_test[:, 1]**2 < 0.5).astype(int)

# Feature map
feature_map = ZZFeatureMap(2)

# Ansatz
ansatz = RealAmplitudes(2, reps=2)

# Create VQC
optimizer = COBYLA(maxiter=100)
sampler = Sampler()

vqc = VQC(
    sampler=sampler,
    feature_map=feature_map,
    ansatz=ansatz,
    optimizer=optimizer,
)

# Train
vqc.fit(X_train, y_train)

# Predict
train_score = vqc.score(X_train, y_train)
test_score = vqc.score(X_test, y_test)

print(f"Training accuracy: {train_score:.2%}")
print(f"Test accuracy: {test_score:.2%}")

# Predictions
predictions = vqc.predict(X_test)
print(f"Sample predictions: {predictions[:5]}")
print(f"True labels: {y_test[:5]}")

Quantum Neural Network (QNN)

from qiskit_machine_learning.neural_networks import SamplerQNN
from qiskit_machine_learning.algorithms import NeuralNetworkClassifier
from qiskit.circuit import QuantumCircuit, Parameter
from qiskit.circuit.library import RealAmplitudes
from qiskit.algorithms.optimizers import COBYLA
from qiskit.primitives import Sampler
import numpy as np

# Create parameterized quantum circuit
def create_qnn_circuit(num_qubits, num_features):
    qc = QuantumCircuit(num_qubits)
    
    # Feature map parameters
    feature_params = [Parameter(f'x{i}') for i in range(num_features)]
    
    # Encode features
    for i, param in enumerate(feature_params):
        if i < num_qubits:
            qc.ry(param, i)
    
    # Variational part
    ansatz = RealAmplitudes(num_qubits, reps=1)
    qc.compose(ansatz, inplace=True)
    
    return qc, feature_params, ansatz.parameters

num_qubits = 2
num_features = 2

qc, feature_params, weight_params = create_qnn_circuit(num_qubits, num_features)

# Create QNN
sampler = Sampler()
qnn = SamplerQNN(
    circuit=qc,
    input_params=feature_params,
    weight_params=weight_params,
    sampler=sampler,
)

# Create classifier
optimizer = COBYLA(maxiter=50)
classifier = NeuralNetworkClassifier(
    neural_network=qnn,
    optimizer=optimizer,
)

# Training data
X_train = np.random.rand(30, 2)
y_train = (X_train[:, 0] > X_train[:, 1]).astype(int)

# Train
classifier.fit(X_train, y_train)

# Test
X_test = np.random.rand(10, 2)
y_test = (X_test[:, 0] > X_test[:, 1]).astype(int)

score = classifier.score(X_test, y_test)
print(f"QNN Classifier accuracy: {score:.2%}")

Noise Modeling and Error Mitigation

Noise Models

from qiskit.providers.aer import AerSimulator
from qiskit.providers.aer.noise import NoiseModel
from qiskit.providers.aer.noise import depolarizing_error, thermal_relaxation_error
from qiskit import QuantumCircuit
import numpy as np

# Create noise model
noise_model = NoiseModel()

# Depolarizing error on single-qubit gates
error_1q = depolarizing_error(0.001, 1)  # 0.1% error
noise_model.add_all_qubit_quantum_error(error_1q, ['u1', 'u2', 'u3', 'rx', 'ry', 'rz'])

# Depolarizing error on two-qubit gates
error_2q = depolarizing_error(0.01, 2)  # 1% error
noise_model.add_all_qubit_quantum_error(error_2q, ['cx', 'cz', 'swap'])

# Thermal relaxation error
# T1 = 50 microseconds, T2 = 70 microseconds, gate_time = 0.1 microseconds
t1 = 50e3  # ns
t2 = 70e3  # ns
gate_time = 100  # ns

error_thermal = thermal_relaxation_error(t1, t2, gate_time)
noise_model.add_all_qubit_quantum_error(error_thermal, ['id'])

# Measurement error
from qiskit.providers.aer.noise import ReadoutError
prob_meas0_prep1 = 0.05  # Prob of measuring 0 when prepared in 1
prob_meas1_prep0 = 0.10  # Prob of measuring 1 when prepared in 0

readout_error = ReadoutError([[1 - prob_meas1_prep0, prob_meas1_prep0],
                               [prob_meas0_prep1, 1 - prob_meas0_prep1]])
noise_model.add_all_qubit_readout_error(readout_error)

print(f"Noise model: {noise_model}")

# Run circuit with noise
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])

# Noiseless simulation
simulator_ideal = AerSimulator()
job_ideal = simulator_ideal.run(qc, shots=1000)
counts_ideal = job_ideal.result().get_counts()

# Noisy simulation
simulator_noisy = AerSimulator(noise_model=noise_model)
job_noisy = simulator_noisy.run(qc, shots=1000)
counts_noisy = job_noisy.result().get_counts()

print(f"\nIdeal results: {counts_ideal}")
print(f"Noisy results: {counts_noisy}")

Zero-Noise Extrapolation (ZNE)

from qiskit import QuantumCircuit, transpile
from qiskit.providers.aer import AerSimulator
from qiskit.providers.aer.noise import NoiseModel, depolarizing_error
import numpy as np
from scipy.optimize import curve_fit

def run_circuit_with_noise(circuit, noise_level, shots=1000):
    """Run circuit with scaled noise."""
    # Create noise model
    noise_model = NoiseModel()
    error = depolarizing_error(noise_level, 1)
    noise_model.add_all_qubit_quantum_error(error, ['u1', 'u2', 'u3'])
    
    # Simulate
    simulator = AerSimulator(noise_model=noise_model)
    job = simulator.run(circuit, shots=shots)
    result = job.result()
    
    # Extract expectation value (simplified)
    counts = result.get_counts()
    expectation = sum(counts.get(bitstring, 0) * (-1)**bitstring.count('1') 
                     for bitstring in counts) / shots
    
    return expectation

def zero_noise_extrapolation(circuit, noise_levels, shots=1000):
    """
    Perform zero-noise extrapolation.
    
    Args:
        circuit: Quantum circuit
        noise_levels: List of noise scaling factors
        shots: Number of shots per simulation
    """
    expectations = []
    
    for noise in noise_levels:
        exp_val = run_circuit_with_noise(circuit, noise, shots)
        expectations.append(exp_val)
        print(f"Noise {noise:.4f}: Expectation = {exp_val:.4f}")
    
    # Fit exponential model: E(λ) = A + B * exp(-C * λ)
    def exp_model(x, a, b, c):
        return a + b * np.exp(-c * x)
    
    # Fit
    popt, _ = curve_fit(exp_model, noise_levels, expectations)
    
    # Extrapolate to zero noise
    zero_noise_value = exp_model(0, *popt)
    
    print(f"\nZero-noise extrapolated value: {zero_noise_value:.4f}")
    
    return zero_noise_value, expectations

# Example circuit
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])

# Run ZNE
noise_levels = np.array([0.001, 0.005, 0.01, 0.02])
zne_value, measured_values = zero_noise_extrapolation(qc, noise_levels)

Measurement Error Mitigation

from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator
from qiskit.providers.aer.noise import NoiseModel, ReadoutError
from qiskit.result import marginal_counts
from qiskit.ignis.mitigation.measurement import (
    complete_meas_cal,
    CompleteMeasFitter
)

# Create readout noise
prob_meas0_prep1 = 0.1
prob_meas1_prep0 = 0.05

readout_error = ReadoutError([[1 - prob_meas1_prep0, prob_meas1_prep0],
                               [prob_meas0_prep1, 1 - prob_meas0_prep1]])

noise_model = NoiseModel()
noise_model.add_all_qubit_readout_error(readout_error)

# Generate calibration circuits
n_qubits = 2
meas_calibs, state_labels = complete_meas_cal(qr=list(range(n_qubits)))

# Run calibration
simulator = AerSimulator(noise_model=noise_model)
cal_results = []

for circuit in meas_calibs:
    job = simulator.run(circuit, shots=1000)
    cal_results.append(job.result())

# Fit the calibration
meas_fitter = CompleteMeasFitter(cal_results, state_labels)

# Get mitigation matrix
print("Calibration matrix:")
print(meas_fitter.cal_matrix)

# Run actual circuit
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])

job = simulator.run(qc, shots=1000)
result = job.result()
noisy_counts = result.get_counts()

# Apply mitigation
mitigated_counts = meas_fitter.filter.apply(noisy_counts)

print(f"\nNoisy counts: {noisy_counts}")
print(f"Mitigated counts: {mitigated_counts}")

Transpilation and Optimization

Basic Transpilation

from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeMontreal
from qiskit.visualization import plot_circuit_layout
import matplotlib.pyplot as plt

# Create circuit
qc = QuantumCircuit(3)
qc.h(0)
qc.cx(0, 1)
qc.cx(1, 2)
qc.cx(0, 2)

# Get fake backend (simulates real hardware)
backend = FakeMontreal()

# Transpile with different optimization levels
for level in range(4):
    transpiled = transpile(qc, backend=backend, optimization_level=level)
    
    print(f"\nOptimization level {level}:")
    print(f"  Depth: {transpiled.depth()}")
    print(f"  Gate count: {len(transpiled.data)}")
    print(f"  CNOT count: {transpiled.count_ops().get('cx', 0)}")

# Best transpilation
best_transpiled = transpile(qc, backend=backend, optimization_level=3)

print(f"\nOriginal circuit:")
print(f"  Depth: {qc.depth()}")
print(f"  Gates: {len(qc.data)}")

print(f"\nTranspiled circuit:")
print(f"  Depth: {best_transpiled.depth()}")
print(f"  Gates: {len(best_transpiled.data)}")

Custom Transpilation Pass

from qiskit import QuantumCircuit
from qiskit.transpiler import PassManager
from qiskit.transpiler.passes import Optimize1qGates, CommutativeCancellation
from qiskit.transpiler.passes import UnitarySynthesis, Unroll3qOrMore

# Create circuit with redundant gates
qc = QuantumCircuit(2)
qc.h(0)
qc.h(0)  # Redundant - cancels previous H
qc.x(1)
qc.x(1)  # Redundant - cancels previous X
qc.cx(0, 1)

print(f"Original circuit depth: {qc.depth()}")
print(f"Original gate count: {len(qc.data)}")

# Create custom pass manager
pm = PassManager()

# Add optimization passes
pm.append(Optimize1qGates())           # Optimize single-qubit gates
pm.append(CommutativeCancellation())   # Cancel commuting gates
pm.append(Unroll3qOrMore())           # Decompose 3+ qubit gates
pm.append(UnitarySynthesis())         # Synthesize unitaries

# Run pass manager
optimized_qc = pm.run(qc)

print(f"\nOptimized circuit depth: {optimized_qc.depth()}")
print(f"Optimized gate count: {len(optimized_qc.data)}")

print("\nOriginal circuit:")
print(qc.draw())

print("\nOptimized circuit:")
print(optimized_qc.draw())

Layout and Routing

from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeMontreal
from qiskit.transpiler import CouplingMap

# Create circuit that requires routing
qc = QuantumCircuit(5)
qc.h(0)
qc.cx(0, 4)  # Long-range connection
qc.cx(1, 3)
qc.cx(2, 4)

# Fake backend with specific topology
backend = FakeMontreal()
coupling_map = backend.configuration().coupling_map

print(f"Backend coupling map: {coupling_map[:10]}...")  # First 10 edges

# Transpile with layout awareness
transpiled = transpile(
    qc,
    backend=backend,
    optimization_level=3,
    seed_transpiler=42  # For reproducibility
)

# Get final layout
final_layout = transpiled.layout.final_index_layout()
print(f"\nFinal qubit layout: {final_layout}")

print(f"\nOriginal circuit:")
print(f"  Depth: {qc.depth()}")
print(f"  CNOT count: {qc.count_ops().get('cx', 0)}")

print(f"\nTranspiled circuit (with routing):")
print(f"  Depth: {transpiled.depth()}")
print(f"  CNOT count: {transpiled.count_ops().get('cx', 0)}")
print(f"  SWAP count: {transpiled.count_ops().get('swap', 0)}")

Quantum Information Theory

Entanglement Measures

from qiskit.quantum_info import Statevector, DensityMatrix, partial_trace
from qiskit.quantum_info import entropy, entanglement_of_formation
from qiskit import QuantumCircuit
import numpy as np

# Create entangled state (Bell state)
qc = QuantumCircuit(2)
qc.h(0)
qc.cx(0, 1)

state = Statevector.from_instruction(qc)
density_matrix = DensityMatrix(state)

print(f"Bell state: {state}")

# Von Neumann entropy (should be 0 for pure states)
entropy_full = entropy(density_matrix)
print(f"\nFull system entropy: {entropy_full:.6f}")

# Reduced density matrix (trace out qubit 1)
rho_0 = partial_trace(density_matrix, [1])
entropy_reduced = entropy(rho_0)
print(f"Reduced density matrix entropy: {entropy_reduced:.6f}")

# Entanglement of formation
# For Bell state, should be 1
eof = entanglement_of_formation(density_matrix)
print(f"Entanglement of formation: {eof:.6f}")

# Compare with separable state
qc_sep = QuantumCircuit(2)
qc_sep.h(0)
qc_sep.h(1)

state_sep = Statevector.from_instruction(qc_sep)
dm_sep = DensityMatrix(state_sep)

rho_0_sep = partial_trace(dm_sep, [1])
entropy_sep = entropy(rho_0_sep)
print(f"\nSeparable state reduced entropy: {entropy_sep:.6f}")

Quantum Channels and Process Tomography

from qiskit.quantum_info import Choi, SuperOp, Kraus
from qiskit import QuantumCircuit
import numpy as np

# Define a quantum channel (amplitude damping)
def amplitude_damping_channel(gamma):
    """
    Amplitude damping channel with damping parameter gamma.
    
    Models energy dissipation.
    """
    K0 = np.array([[1, 0], [0, np.sqrt(1 - gamma)]])
    K1 = np.array([[0, np.sqrt(gamma)], [0, 0]])
    
    return Kraus([K0, K1])

# Create channel
gamma = 0.3
channel = amplitude_damping_channel(gamma)

print(f"Amplitude damping channel (γ={gamma}):")
print(f"Number of Kraus operators: {len(channel)}")

# Convert to different representations
superop = SuperOp(channel)
choi = Choi(channel)

print(f"\nSuperoperator shape: {superop.dim}")
print(f"Choi matrix shape: {choi.dim}")

# Apply channel to a state
from qiskit.quantum_info import Statevector, DensityMatrix

# Initial state |1⟩
state = Statevector([0, 1])
dm = DensityMatrix(state)

# Apply channel
dm_evolved = dm.evolve(channel)

print(f"\nInitial state: {state}")
print(f"After channel: {dm_evolved}")

# Measure fidelity
from qiskit.quantum_info import state_fidelity
fidelity = state_fidelity(dm, dm_evolved)
print(f"Fidelity: {fidelity:.6f}")

Quantum State Tomography

from qiskit.quantum_info import Statevector, DensityMatrix
from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator
from qiskit.quantum_info.states import state_fidelity
import numpy as np

def perform_state_tomography(qc, shots=1000):
    """
    Simplified quantum state tomography.
    
    Measures in X, Y, Z bases to reconstruct density matrix.
    """
    simulator = AerSimulator()
    
    # Measurement circuits in different bases
    measurements = {
        'Z': QuantumCircuit(qc.num_qubits, qc.num_qubits),
        'X': QuantumCircuit(qc.num_qubits, qc.num_qubits),
        'Y': QuantumCircuit(qc.num_qubits, qc.num_qubits)
    }
    
    # X basis: apply H before measurement
    measurements['X'].h(range(qc.num_qubits))
    
    # Y basis: apply S†H before measurement
    measurements['Y'].sdg(range(qc.num_qubits))
    measurements['Y'].h(range(qc.num_qubits))
    
    # Measure all
    for basis_circ in measurements.values():
        basis_circ.measure(range(qc.num_qubits), range(qc.num_qubits))
    
    # Run measurements
    results = {}
    for basis, meas_circ in measurements.items():
        full_circ = qc.copy()
        full_circ.compose(meas_circ, inplace=True)
        
        job = simulator.run(full_circ, shots=shots)
        results[basis] = job.result().get_counts()
    
    print(f"Z-basis measurements: {results['Z']}")
    print(f"X-basis measurements: {results['X']}")
    print(f"Y-basis measurements: {results['Y']}")
    
    # Simplified reconstruction (for single qubit)
    if qc.num_qubits == 1:
        # Extract Pauli expectation values
        z_exp = (results['Z'].get('0', 0) - results['Z'].get('1', 0)) / shots
        x_exp = (results['X'].get('0', 0) - results['X'].get('1', 0)) / shots
        y_exp = (results['Y'].get('0', 0) - results['Y'].get('1', 0)) / shots
        
        # Reconstruct density matrix: ρ = (I + x⟨X⟩ + y⟨Y⟩ + z⟨Z⟩)/2
        rho = np.array([
            [0.5 + 0.5*z_exp, 0.5*x_exp - 0.5j*y_exp],
            [0.5*x_exp + 0.5j*y_exp, 0.5 - 0.5*z_exp]
        ])
        
        return DensityMatrix(rho)
    
    return None

# Test on a known state
qc = QuantumCircuit(1)
qc.ry(np.pi/3, 0)  # Rotate to create superposition

# True state
true_state = Statevector.from_instruction(qc)
true_dm = DensityMatrix(true_state)

# Tomography
reconstructed_dm = perform_state_tomography(qc, shots=10000)

if reconstructed_dm is not None:
    fidelity = state_fidelity(true_dm, reconstructed_dm)
    print(f"\nReconstruction fidelity: {fidelity:.6f}")
    print(f"\nTrue density matrix:\n{np.array(true_dm)}")
    print(f"\nReconstructed density matrix:\n{np.array(reconstructed_dm)}")

Visualization

Circuit Visualization

from qiskit import QuantumCircuit
from qiskit.visualization import circuit_drawer
import matplotlib.pyplot as plt

# Create complex circuit
qc = QuantumCircuit(3, 3)
qc.h(0)
qc.cx(0, 1)
qc.cx(1, 2)
qc.barrier()
qc.measure([0, 1, 2], [0, 1, 2])

# Different drawing styles
print("Text representation:")
print(qc.draw(output='text'))

# Matplotlib style (most common)
print("\nMatplotlib style:")
qc.draw(output='mpl')
plt.show()

# LaTeX style (for publications)
# qc.draw(output='latex')

# With gate labels
qc_labeled = QuantumCircuit(2, 2)
qc_labeled.h(0)
qc_labeled.cx(0, 1)
qc_labeled.measure_all()

qc_labeled.draw(output='mpl', style={'name': 'bw'})
plt.show()

Result Visualization

from qiskit import QuantumCircuit
from qiskit.providers.aer import AerSimulator
from qiskit.visualization import plot_histogram, plot_bloch_multivector
from qiskit.quantum_info import Statevector
import matplotlib.pyplot as plt

# Run circuit
qc = QuantumCircuit(2, 2)
qc.h(0)
qc.cx(0, 1)
qc.measure([0, 1], [0, 1])

simulator = AerSimulator()
job = simulator.run(qc, shots=1000)
counts = job.result().get_counts()

# Histogram
plot_histogram(counts, title='Bell State Measurement')
plt.show()

# Multiple result comparison
qc2 = QuantumCircuit(2, 2)
qc2.h(0)
qc2.h(1)
qc2.measure([0, 1], [0, 1])

job2 = simulator.run(qc2, shots=1000)
counts2 = job2.result().get_counts()

plot_histogram([counts, counts2], 
               legend=['Bell State', 'Product State'],
               title='State Comparison')
plt.show()

# Bloch sphere visualization
qc_bloch = QuantumCircuit(1)
qc_bloch.ry(np.pi/4, 0)

state = Statevector.from_instruction(qc_bloch)
plot_bloch_multivector(state)
plt.show()

State Visualization

from qiskit.quantum_info import Statevector, DensityMatrix
from qiskit.visualization import plot_state_qsphere, plot_state_city
from qiskit.visualization import plot_state_hinton, plot_state_paulivec
import matplotlib.pyplot as plt

# Create an interesting state
from qiskit import QuantumCircuit
qc = QuantumCircuit(2)
qc.h(0)
qc.ry(np.pi/4, 1)
qc.cx(0, 1)

state = Statevector.from_instruction(qc)

# Q-sphere
plot_state_qsphere(state, title='Q-sphere')
plt.show()

# City plot
plot_state_city(state, title='State City')
plt.show()

# Hinton plot
dm = DensityMatrix(state)
plot_state_hinton(dm, title='Density Matrix')
plt.show()

# Pauli vector representation
plot_state_paulivec(state, title='Pauli Vector')
plt.show()

Practical Workflows

Complete VQE Workflow for Molecule

from qiskit_nature.second_q.drivers import PySCFDriver
from qiskit_nature.second_q.mappers import JordanWignerMapper
from qiskit_nature.second_q.circuit.library import UCCSD, HartreeFock
from qiskit.algorithms import VQE
from qiskit.algorithms.optimizers import SLSQP
from qiskit.primitives import Estimator
import numpy as np

def calculate_molecule_energy(atom_string, basis='sto3g', charge=0, spin=0):
    """
    Complete workflow for molecular energy calculation.
    
    Args:
        atom_string: Atomic coordinates (e.g., 'H 0 0 0; H 0 0 0.735')
        basis: Basis set
        charge: Molecular charge
        spin: Spin multiplicity
    """
    print(f"Calculating energy for: {atom_string}")
    print(f"Basis: {basis}, Charge: {charge}, Spin: {spin}\n")
    
    # 1. Setup driver
    driver = PySCFDriver(
        atom=atom_string,
        basis=basis,
        charge=charge,
        spin=spin
    )
    
    # 2. Get electronic structure problem
    problem = driver.run()
    
    # 3. Setup mapper
    mapper = JordanWignerMapper()
    
    # 4. Get Hamiltonian
    hamiltonian = problem.hamiltonian.second_q_op()
    qubit_op = mapper.map(hamiltonian)
    
    print(f"Number of qubits: {qubit_op.num_qubits}")
    print(f"Number of Hamiltonian terms: {len(qubit_op)}")
    
    # 5. Setup initial state and ansatz
    num_particles = problem.num_particles
    num_spatial_orbitals = problem.num_spatial_orbitals
    
    init_state = HartreeFock(
        num_spatial_orbitals=num_spatial_orbitals,
        num_particles=num_particles,
        qubit_mapper=mapper
    )
    
    ansatz = UCCSD(
        num_spatial_orbitals=num_spatial_orbitals,
        num_particles=num_particles,
        qubit_mapper=mapper,
        initial_state=init_state
    )
    
    print(f"Ansatz circuit depth: {ansatz.depth()}")
    print(f"Number of parameters: {ansatz.num_parameters}\n")
    
    # 6. Run VQE
    optimizer = SLSQP(maxiter=100)
    estimator = Estimator()
    
    vqe = VQE(estimator, ansatz, optimizer)
    result = vqe.compute_minimum_eigenvalue(qubit_op)
    
    # 7. Extract results
    vqe_energy = result.eigenvalue
    hf_energy = problem.reference_energy
    
    print(f"Hartree-Fock energy: {hf_energy:.6f} Ha")
    print(f"VQE energy: {vqe_energy:.6f} Ha")
    print(f"Correlation energy: {vqe_energy - hf_energy:.6f} Ha")
    print(f"Optimizer evaluations: {result.cost_function_evals}")
    
    return {
        'vqe_energy': vqe_energy,
        'hf_energy': hf_energy,
        'correlation': vqe_energy - hf_energy,
        'optimal_parameters': result.optimal_parameters,
        'num_qubits': qubit_op.num_qubits
    }

# Example: H2 molecule
results = calculate_molecule_energy('H 0 0 0; H 0 0 0.735')

Quantum Circuit Optimization Pipeline

from qiskit import QuantumCircuit, transpile
from qiskit.providers.fake_provider import FakeMontreal
from qiskit.transpiler import PassManager, CouplingMap
from qiskit.transpiler.passes import *
import matplotlib.pyplot as plt

def optimize_circuit_for_hardware(qc, backend=None, optimization_level=3):
    """
    Complete circuit optimization pipeline.
    
    Args:
        qc: Input quantum circuit
        backend: Target backend (or None for generic optimization)
        optimization_level: 0-3
    """
    print(f"Original circuit:")
    print(f"  Qubits: {qc.num_qubits}")
    print(f"  Depth: {qc.depth()}")
    print(f"  Gate count: {len(qc.data)}")
    print(f"  Operations: {qc.count_ops()}\n")
    
    if backend is None:
        backend = FakeMontreal()
    
    # Standard transpilation
    transpiled = transpile(
        qc,
        backend=backend,
        optimization_level=optimization_level,
        seed_transpiler=42
    )
    
    print(f"After transpilation (level {optimization_level}):")
    print(f"  Depth: {transpiled.depth()}")
    print(f"  Gate count: {len(transpiled.data)}")
    print(f"  Operations: {transpiled.count_ops()}")
    print(f"  SWAP gates: {transpiled.count_ops().get('swap', 0)}\n")
    
    # Custom optimization passes
    pm = PassManager()
    
    # Add passes
    pm.append(Optimize1qGates())
    pm.append(CommutativeCancellation())
    pm.append(CXCancellation())
    
    further_optimized = pm.run(transpiled)
    
    print(f"After custom optimization:")
    print(f"  Depth: {further_optimized.depth()}")
    print(f"  Gate count: {len(further_optimized.data)}")
    print(f"  Operations: {further_optimized.count_ops()}\n")
    
    # Calculate reduction
    depth_reduction = (1 - further_optimized.depth() / qc.depth()) * 100
    gate_reduction = (1 - len(further_optimized.data) / len(qc.data)) * 100
    
    print(f"Optimization results:")
    print(f"  Depth reduction: {depth_reduction:.1f}%")
    print(f"  Gate count reduction: {gate_reduction:.1f}%")
    
    return further_optimized

# Example: Complex circuit
qc = QuantumCircuit(4)
qc.h(range(4))
for i in range(3):
    qc.cx(i, i+1)
qc.barrier()
for i in range(4):
    qc.ry(np.pi/4, i)
qc.barrier()
for i in range(2):
    qc.cx(i, i+2)

optimized = optimize_circuit_for_hardware(qc)

Quantum Algorithm Benchmarking

from qiskit import QuantumCircuit
from qiskit.algorithms import VQE, QAOA
from qiskit.algorithms.optimizers import SLSQP, COBYLA, SPSA
from qiskit.circuit.library import RealAmplitudes
from qiskit.primitives import Estimator
from qiskit.quantum_info import SparsePauliOp
import time
import numpy as np

def benchmark_vqe_optimizers(hamiltonian, ansatz, optimizers_dict, trials=3):
    """
    Benchmark different optimizers for VQE.
    
    Args:
        hamiltonian: Problem Hamiltonian
        ansatz: Variational ansatz
        optimizers_dict: Dict of optimizer name -> optimizer instance
        trials: Number of trials per optimizer
    """
    results = {}
    
    for opt_name, optimizer in optimizers_dict.items():
        print(f"\nBenchmarking {opt_name}...")
        
        trial_results = []
        
        for trial in range(trials):
            estimator = Estimator()
            vqe = VQE(estimator, ansatz, optimizer)
            
            start_time = time.time()
            result = vqe.compute_minimum_eigenvalue(hamiltonian)
            elapsed_time = time.time() - start_time
            
            trial_results.append({
                'energy': result.eigenvalue,
                'time': elapsed_time,
                'evals': result.cost_function_evals
            })
            
            print(f"  Trial {trial + 1}: E = {result.eigenvalue:.6f}, "
                  f"Time = {elapsed_time:.2f}s, Evals = {result.cost_function_evals}")
        
        # Aggregate results
        energies = [r['energy'] for r in trial_results]
        times = [r['time'] for r in trial_results]
        evals = [r['evals'] for r in trial_results]
        
        results[opt_name] = {
            'mean_energy': np.mean(energies),
            'std_energy': np.std(energies),
            'mean_time': np.mean(times),
            'mean_evals': np.mean(evals),
            'best_energy': min(energies)
        }
    
    # Print summary
    print("\n" + "="*60)
    print("BENCHMARK SUMMARY")
    print("="*60)
    print(f"{'Optimizer':<15} {'Best Energy':>12} {'Mean Time':>12} {'Mean Evals':>12}")
    print("-"*60)
    
    for opt_name, res in results.items():
        print(f"{opt_name:<15} {res['best_energy']:>12.6f} "
              f"{res['mean_time']:>12.2f}s {res['mean_evals']:>12.0f}")
    
    return results

# Example: Benchmark for simple Hamiltonian
hamiltonian = SparsePauliOp(['ZZ', 'XI', 'IX'], coeffs=[1.0, -0.5, -0.5])
ansatz = RealAmplitudes(num_qubits=2, reps=2)

optimizers = {
    'SLSQP': SLSQP(maxiter=100),
    'COBYLA': COBYLA(maxiter=100),
    'SPSA': SPSA(maxiter=100)
}

benchmark_results = benchmark_vqe_optimizers(hamiltonian, ansatz, optimizers, trials=3)