An open source library for interacting with quantum computing devices on Amazon Braket
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Advanced quantum computing paradigms including Analog Hamiltonian Simulation (AHS), quantum annealing, pulse-level control, error mitigation, and experimental capabilities.
# Analog Hamiltonian Simulation
from braket.ahs import (
AnalogHamiltonianSimulation, AtomArrangement, AtomArrangementItem, SiteType,
Canvas, DiscretizationProperties, DrivingField, Field, Hamiltonian,
LocalDetuning, Pattern, ShiftingField
)
# Quantum Annealing
from braket.annealing import Problem, ProblemType
# Pulse Control
from braket.pulse import (
Frame, Port, PulseSequence, ArbitraryWaveform, ConstantWaveform,
DragGaussianWaveform, ErfSquareWaveform, GaussianWaveform
)
# Error Mitigation
from braket.error_mitigation import Debias, ErrorMitigation
# Experimental Capabilities
from braket.experimental_capabilities import EnableExperimentalCapabilityfrom braket.ahs import AnalogHamiltonianSimulation, Hamiltonian, AtomArrangement
import numpy as np
class AnalogHamiltonianSimulation:
"""Main AHS program for neutral atom quantum computing."""
def __init__(self):
"""Initialize empty AHS program."""
self.hamiltonian = None
self.atom_arrangement = None
self.discretization_properties = None
@classmethod
def create(
cls,
atom_arrangement: 'AtomArrangement',
hamiltonian: 'Hamiltonian',
discretization_properties: 'DiscretizationProperties' = None
) -> 'AnalogHamiltonianSimulation':
"""
Create AHS program with atom arrangement and Hamiltonian.
Args:
atom_arrangement: Spatial arrangement of neutral atoms
hamiltonian: Time-dependent Hamiltonian specification
discretization_properties: Time discretization settings
Returns:
AnalogHamiltonianSimulation: Complete AHS program
"""
pass
def to_ir(self) -> dict:
"""
Convert to intermediate representation for device execution.
Returns:
dict: AHS program in device-compatible format
"""
pass
class AtomArrangement:
"""Atom position arrangement for AHS."""
def __init__(self):
"""Initialize empty atom arrangement."""
self.sites = []
def add(self, coordinate: tuple[float, float], site_type: 'SiteType' = None) -> 'AtomArrangement':
"""
Add atom site to arrangement.
Args:
coordinate: (x, y) position in micrometers
site_type: Type of site (filled or vacant)
Returns:
AtomArrangement: Self for method chaining
"""
pass
def add_item(self, item: 'AtomArrangementItem') -> 'AtomArrangement':
"""
Add pre-configured arrangement item.
Args:
item: Atom arrangement item
Returns:
AtomArrangement: Self for method chaining
"""
pass
@property
def coordinate_list(self) -> list[tuple[float, float]]:
"""Get list of atom coordinates."""
pass
def visualize(self) -> 'Canvas':
"""
Create visualization of atom arrangement.
Returns:
Canvas: Visual representation of atom layout
"""
pass
class AtomArrangementItem:
"""Individual atom arrangement item."""
def __init__(self, coordinate: tuple[float, float], site_type: 'SiteType'):
"""
Initialize atom arrangement item.
Args:
coordinate: (x, y) position in micrometers
site_type: Type of site
"""
self.coordinate = coordinate
self.site_type = site_type
class SiteType:
"""Site type enumeration for atom arrangements."""
FILLED = "filled"
VACANT = "vacant"
# AHS program examples
def create_rydberg_blockade_program(lattice_spacing: float = 5.0) -> AnalogHamiltonianSimulation:
"""
Create AHS program for Rydberg blockade physics.
Args:
lattice_spacing: Spacing between atoms in micrometers
Returns:
AnalogHamiltonianSimulation: Rydberg blockade AHS program
"""
# Create square lattice of atoms
arrangement = AtomArrangement()
n_atoms_per_side = 3
for i in range(n_atoms_per_side):
for j in range(n_atoms_per_side):
x = i * lattice_spacing
y = j * lattice_spacing
arrangement.add((x, y), SiteType.FILLED)
# Create time-dependent Hamiltonian
# H = Ω(t)/2 ∑ᵢ (σˣⁱ) - Δ(t) ∑ᵢ nᵢ + ∑ᵢⱼ V_ij nᵢnⱼ
hamiltonian = create_rydberg_hamiltonian()
# Time evolution settings
discretization = DiscretizationProperties(
time_step=1e-7, # 0.1 microseconds
time_series_precision=1e-9
)
return AnalogHamiltonianSimulation.create(
arrangement, hamiltonian, discretization
)
def create_quantum_annealing_ahs_program() -> AnalogHamiltonianSimulation:
"""
Create AHS program for quantum annealing-like evolution.
Returns:
AnalogHamiltonianSimulation: Quantum annealing AHS program
"""
# Linear chain for transverse-field Ising model
arrangement = AtomArrangement()
chain_length = 5
spacing = 8.0 # micrometers
for i in range(chain_length):
arrangement.add((i * spacing, 0.0), SiteType.FILLED)
# Create annealing schedule
total_time = 2.0 # microseconds
# Driving field (transverse field analog)
driving_amplitude = create_annealing_schedule(
initial_value=2*np.pi * 10, # MHz
final_value=0.0,
total_time=total_time
)
# Detuning (longitudinal field)
detuning = create_annealing_schedule(
initial_value=0.0,
final_value=2*np.pi * 5, # MHz
total_time=total_time
)
hamiltonian = Hamiltonian()
hamiltonian.driving_field = DrivingField(
amplitude=driving_amplitude,
phase=Pattern.constant(0.0),
detuning=detuning
)
return AnalogHamiltonianSimulation.create(arrangement, hamiltonian)
def analyze_ahs_program(ahs_program: AnalogHamiltonianSimulation) -> dict:
"""
Analyze AHS program for physics insights and optimization.
Args:
ahs_program: AHS program to analyze
Returns:
dict: Comprehensive program analysis
"""
analysis = {
'atom_configuration': {},
'hamiltonian_properties': {},
'time_evolution': {},
'physics_regime': {},
'computational_complexity': {}
}
# Analyze atom arrangement
coords = ahs_program.atom_arrangement.coordinate_list
n_atoms = len(coords)
analysis['atom_configuration'] = {
'atom_count': n_atoms,
'spatial_dimension': 2, # 2D arrangements
'lattice_spacing': calculate_average_spacing(coords),
'geometry': identify_lattice_geometry(coords),
'coordination_number': calculate_coordination_numbers(coords)
}
# Analyze Hamiltonian
hamiltonian = ahs_program.hamiltonian
analysis['hamiltonian_properties'] = {
'has_driving_field': hamiltonian.driving_field is not None,
'has_local_detuning': hasattr(hamiltonian, 'local_detuning') and hamiltonian.local_detuning is not None,
'interaction_range': estimate_interaction_range(coords),
'rydberg_blockade_radius': calculate_blockade_radius(coords)
}
# Physics regime analysis
if analysis['hamiltonian_properties']['has_driving_field']:
analysis['physics_regime']['type'] = 'Rydberg blockade'
analysis['physics_regime']['phenomena'] = [
'Quantum many-body scarring',
'Rydberg crystallization',
'Quantum phase transitions'
]
else:
analysis['physics_regime']['type'] = 'Ising-like'
analysis['physics_regime']['phenomena'] = [
'Ground state optimization',
'Quantum annealing',
'Combinatorial optimization'
]
# Computational complexity
hilbert_space_size = 2 ** n_atoms # Each atom can be |0⟩ or |r⟩
analysis['computational_complexity'] = {
'hilbert_space_size': hilbert_space_size,
'classical_simulation_feasible': n_atoms <= 20,
'approximate_methods_needed': n_atoms > 15,
'estimated_execution_time': estimate_ahs_execution_time(ahs_program)
}
return analysis
def calculate_average_spacing(coordinates: list[tuple[float, float]]) -> float:
"""Calculate average nearest-neighbor spacing."""
if len(coordinates) < 2:
return 0.0
total_distance = 0.0
count = 0
for i, (x1, y1) in enumerate(coordinates):
min_distance = float('inf')
for j, (x2, y2) in enumerate(coordinates):
if i != j:
distance = np.sqrt((x2-x1)**2 + (y2-y1)**2)
min_distance = min(min_distance, distance)
if min_distance < float('inf'):
total_distance += min_distance
count += 1
return total_distance / count if count > 0 else 0.0from braket.ahs import Hamiltonian, DrivingField, LocalDetuning, Pattern
from braket.timings import TimeSeries
class Hamiltonian:
"""AHS Hamiltonian specification."""
def __init__(self):
"""Initialize empty Hamiltonian."""
self.driving_field = None
self.local_detuning = None
def add_driving_field(self, driving_field: 'DrivingField') -> 'Hamiltonian':
"""
Add global driving field term.
Args:
driving_field: Global Rabi driving field
Returns:
Hamiltonian: Self for method chaining
"""
self.driving_field = driving_field
return self
def add_local_detuning(self, local_detuning: 'LocalDetuning') -> 'Hamiltonian':
"""
Add local detuning field.
Args:
local_detuning: Site-dependent detuning field
Returns:
Hamiltonian: Self for method chaining
"""
self.local_detuning = local_detuning
return self
class DrivingField(Field):
"""Hamiltonian driving field for Rabi oscillations."""
def __init__(
self,
amplitude: 'Pattern',
phase: 'Pattern',
detuning: 'Pattern'
):
"""
Initialize driving field.
Args:
amplitude: Time-dependent Rabi frequency Ω(t)
phase: Time-dependent phase φ(t)
detuning: Time-dependent detuning Δ(t)
"""
self.amplitude = amplitude
self.phase = phase
self.detuning = detuning
class LocalDetuning(Field):
"""Local detuning field for site-dependent energy shifts."""
def __init__(self, magnitude: 'Pattern'):
"""
Initialize local detuning field.
Args:
magnitude: Spatially-dependent detuning magnitude
"""
self.magnitude = magnitude
class Pattern:
"""Time-dependent pattern for AHS fields."""
@staticmethod
def constant(value: float) -> 'Pattern':
"""
Create constant pattern.
Args:
value: Constant value
Returns:
Pattern: Constant pattern
"""
pass
@staticmethod
def linear(start_value: float, end_value: float, duration: float) -> 'Pattern':
"""
Create linear interpolation pattern.
Args:
start_value: Initial value
end_value: Final value
duration: Pattern duration
Returns:
Pattern: Linear interpolation pattern
"""
pass
@staticmethod
def from_time_series(time_series: TimeSeries) -> 'Pattern':
"""
Create pattern from time series data.
Args:
time_series: Time-dependent values
Returns:
Pattern: Pattern from time series
"""
pass
def create_rydberg_hamiltonian() -> Hamiltonian:
"""
Create typical Rydberg Hamiltonian for quantum simulation.
Returns:
Hamiltonian: Rydberg blockade Hamiltonian
"""
hamiltonian = Hamiltonian()
# Time-dependent Rabi frequency (adiabatic ramp)
omega_max = 2*np.pi * 15 # 15 MHz
ramp_time = 1.0 # microseconds
hold_time = 0.5 # microseconds
# Create piecewise linear amplitude
amplitude_points = [
(0.0, 0.0), # Start at zero
(ramp_time/4, omega_max), # Ramp up
(3*ramp_time/4, omega_max), # Hold
(ramp_time, 0.0) # Ramp down
]
amplitude_series = TimeSeries()
for time, value in amplitude_points:
amplitude_series.add_point(time, value)
amplitude_pattern = Pattern.from_time_series(amplitude_series)
# Constant phase and detuning
phase_pattern = Pattern.constant(0.0)
detuning_pattern = Pattern.constant(0.0)
# Add driving field
driving_field = DrivingField(
amplitude=amplitude_pattern,
phase=phase_pattern,
detuning=detuning_pattern
)
hamiltonian.add_driving_field(driving_field)
return hamiltonian
def create_annealing_schedule(initial_value: float, final_value: float, total_time: float) -> Pattern:
"""
Create annealing schedule pattern for AHS.
Args:
initial_value: Starting parameter value
final_value: Ending parameter value
total_time: Total annealing time
Returns:
Pattern: Annealing schedule pattern
"""
# Create smooth S-curve annealing schedule
n_points = 100
times = np.linspace(0, total_time, n_points)
# S-curve using tanh function
s_values = []
for t in times:
s = (np.tanh(4 * (t/total_time - 0.5)) + 1) / 2 # Sigmoid from 0 to 1
value = initial_value + s * (final_value - initial_value)
s_values.append(value)
# Create time series
time_series = TimeSeries()
for t, v in zip(times, s_values):
time_series.add_point(t, v)
return Pattern.from_time_series(time_series)from braket.annealing import Problem, ProblemType
from enum import Enum
class ProblemType(Enum):
"""Types of annealing problems."""
QUBO = "QUBO"
ISING = "ISING"
class Problem:
"""Annealing problem specification."""
def __init__(self, problem_type: ProblemType):
"""
Initialize annealing problem.
Args:
problem_type: Type of optimization problem (QUBO or Ising)
"""
self.problem_type = problem_type
self.linear = {} # Linear terms
self.quadratic = {} # Quadratic terms
def add_linear(self, variable: int, coefficient: float) -> 'Problem':
"""
Add linear term to problem.
Args:
variable: Variable index
coefficient: Linear coefficient
Returns:
Problem: Self for method chaining
"""
self.linear[variable] = coefficient
return self
def add_quadratic(self, var1: int, var2: int, coefficient: float) -> 'Problem':
"""
Add quadratic term to problem.
Args:
var1: First variable index
var2: Second variable index
coefficient: Quadratic coefficient
Returns:
Problem: Self for method chaining
"""
self.quadratic[(var1, var2)] = coefficient
return self
def to_dict(self) -> dict:
"""
Convert problem to dictionary representation.
Returns:
dict: Problem in dictionary format
"""
return {
'type': self.problem_type.value,
'linear': self.linear,
'quadratic': self.quadratic
}
# Annealing examples
def create_max_cut_problem(graph_edges: list[tuple[int, int]]) -> Problem:
"""
Create Max-Cut problem for quantum annealing.
Args:
graph_edges: List of graph edges as (node1, node2) pairs
Returns:
Problem: Max-Cut QUBO formulation
"""
problem = Problem(ProblemType.QUBO)
# Max-Cut QUBO formulation: maximize ∑ᵢⱼ wᵢⱼ xᵢ(1-xⱼ) + wᵢⱼ(1-xᵢ)xⱼ
# Equivalent to: minimize -∑ᵢⱼ wᵢⱼ(xᵢ + xⱼ - 2xᵢxⱼ)
# Assume unit weights for simplicity
nodes = set()
for i, j in graph_edges:
nodes.add(i)
nodes.add(j)
# Linear terms: -wᵢⱼ for each edge (i,j)
linear_coeffs = {}
for i, j in graph_edges:
linear_coeffs[i] = linear_coeffs.get(i, 0) - 1
linear_coeffs[j] = linear_coeffs.get(j, 0) - 1
for node, coeff in linear_coeffs.items():
problem.add_linear(node, coeff)
# Quadratic terms: +2wᵢⱼ for each edge (i,j)
for i, j in graph_edges:
problem.add_quadratic(i, j, 2.0)
return problem
def create_number_partitioning_problem(numbers: list[int]) -> Problem:
"""
Create number partitioning problem for quantum annealing.
Args:
numbers: List of numbers to partition into equal-sum sets
Returns:
Problem: Number partitioning QUBO formulation
"""
problem = Problem(ProblemType.QUBO)
# Number partitioning: minimize (∑ᵢ aᵢxᵢ - S/2)²
# where S = ∑ᵢ aᵢ is total sum
S = sum(numbers)
target = S // 2 # Target sum for each partition
# Expand: (∑ᵢ aᵢxᵢ - target)² = ∑ᵢ aᵢ²xᵢ + 2∑ᵢⱼ aᵢaⱼxᵢxⱼ - 2target∑ᵢ aᵢxᵢ + target²
# Ignore constant target² term
# Linear terms: aᵢ² - 2target·aᵢ
for i, a in enumerate(numbers):
linear_coeff = a*a - 2*target*a
problem.add_linear(i, linear_coeff)
# Quadratic terms: 2aᵢaⱼ for i < j
for i in range(len(numbers)):
for j in range(i+1, len(numbers)):
quadratic_coeff = 2 * numbers[i] * numbers[j]
problem.add_quadratic(i, j, quadratic_coeff)
return problem
def create_portfolio_optimization_problem(returns: list[float], risks: list[list[float]], risk_penalty: float = 1.0) -> Problem:
"""
Create portfolio optimization problem for quantum annealing.
Args:
returns: Expected returns for each asset
risks: Risk covariance matrix
risk_penalty: Risk penalty parameter λ
Returns:
Problem: Portfolio optimization QUBO formulation
"""
problem = Problem(ProblemType.QUBO)
n_assets = len(returns)
# Portfolio optimization: maximize ∑ᵢ rᵢxᵢ - λ ∑ᵢⱼ σᵢⱼxᵢxⱼ
# Convert to minimization: minimize -∑ᵢ rᵢxᵢ + λ ∑ᵢⱼ σᵢⱼxᵢxⱼ
# Linear terms: -rᵢ (negative expected returns)
for i, r in enumerate(returns):
problem.add_linear(i, -r)
# Quadratic terms: λσᵢⱼ (risk penalties)
for i in range(n_assets):
for j in range(i, n_assets):
if i == j:
# Diagonal terms (variance)
risk_coeff = risk_penalty * risks[i][j]
problem.add_linear(i, risk_coeff) # Add to diagonal
else:
# Off-diagonal terms (covariance)
risk_coeff = risk_penalty * risks[i][j]
problem.add_quadratic(i, j, 2 * risk_coeff) # Factor of 2 for symmetry
return problem
def analyze_annealing_problem(problem: Problem) -> dict:
"""
Analyze quantum annealing problem for optimization insights.
Args:
problem: Annealing problem to analyze
Returns:
dict: Problem analysis and optimization recommendations
"""
analysis = {
'problem_structure': {},
'complexity_metrics': {},
'annealing_parameters': {},
'optimization_difficulty': {}
}
# Analyze problem structure
n_variables = len(set(list(problem.linear.keys()) +
[var for pair in problem.quadratic.keys() for var in pair]))
n_linear_terms = len(problem.linear)
n_quadratic_terms = len(problem.quadratic)
analysis['problem_structure'] = {
'problem_type': problem.problem_type.value,
'variable_count': n_variables,
'linear_terms': n_linear_terms,
'quadratic_terms': n_quadratic_terms,
'density': n_quadratic_terms / (n_variables * (n_variables - 1) / 2) if n_variables > 1 else 0
}
# Complexity analysis
coefficient_magnitudes = (list(problem.linear.values()) +
list(problem.quadratic.values()))
analysis['complexity_metrics'] = {
'coefficient_range': (min(coefficient_magnitudes), max(coefficient_magnitudes)),
'coefficient_std': np.std(coefficient_magnitudes),
'sparsity': 1 - (n_linear_terms + n_quadratic_terms) / (n_variables + n_variables**2/2),
'conditioning': max(coefficient_magnitudes) / min(abs(c) for c in coefficient_magnitudes if c != 0)
}
# Annealing parameter recommendations
if analysis['complexity_metrics']['conditioning'] > 100:
recommended_annealing_time = 'Long (>100μs)'
recommended_schedule = 'Slow linear or exponential'
else:
recommended_annealing_time = 'Standard (20-50μs)'
recommended_schedule = 'Linear or fast exponential'
analysis['annealing_parameters'] = {
'recommended_annealing_time': recommended_annealing_time,
'recommended_schedule': recommended_schedule,
'suggested_repetitions': max(1000, 10 * n_variables),
'post_processing': 'Consider classical refinement for large problems'
}
return analysisfrom braket.pulse import PulseSequence, Frame, Port
import numpy as np
class PulseSequence:
"""Sequence of pulse operations for direct hardware control."""
def __init__(self):
"""Initialize empty pulse sequence."""
self.operations = []
self.duration = 0.0
def play(self, frame: 'Frame', waveform: 'Waveform') -> 'PulseSequence':
"""
Play waveform on specified frame.
Args:
frame: Target frame for pulse
waveform: Pulse waveform to play
Returns:
PulseSequence: Self for method chaining
"""
pass
def delay(self, frame: 'Frame', duration: float) -> 'PulseSequence':
"""
Add delay on frame.
Args:
frame: Target frame
duration: Delay duration in seconds
Returns:
PulseSequence: Self for method chaining
"""
pass
def shift_frequency(self, frame: 'Frame', frequency: float) -> 'PulseSequence':
"""
Shift frame frequency.
Args:
frame: Target frame
frequency: Frequency shift in Hz
Returns:
PulseSequence: Self for method chaining
"""
pass
def set_phase(self, frame: 'Frame', phase: float) -> 'PulseSequence':
"""
Set frame phase.
Args:
frame: Target frame
phase: Phase in radians
Returns:
PulseSequence: Self for method chaining
"""
pass
def barrier(self, frames: list['Frame']) -> 'PulseSequence':
"""
Add synchronization barrier across frames.
Args:
frames: Frames to synchronize
Returns:
PulseSequence: Self for method chaining
"""
pass
class Frame:
"""Pulse frame definition for frequency and phase tracking."""
def __init__(
self,
frame_id: str,
port: 'Port',
frequency: float,
phase: float = 0.0
):
"""
Initialize pulse frame.
Args:
frame_id: Unique frame identifier
port: Associated hardware port
frequency: Frame frequency in Hz
phase: Initial phase in radians
"""
self.frame_id = frame_id
self.port = port
self.frequency = frequency
self.phase = phase
class Port:
"""Hardware port specification."""
def __init__(self, port_id: str, dt: float):
"""
Initialize hardware port.
Args:
port_id: Unique port identifier
dt: Port time resolution in seconds
"""
self.port_id = port_id
self.dt = dt
# Waveform definitions
class GaussianWaveform:
"""Gaussian pulse waveform."""
def __init__(
self,
length: float,
amplitude: float,
sigma: float
):
"""
Initialize Gaussian waveform.
Args:
length: Pulse length in seconds
amplitude: Peak amplitude
sigma: Gaussian width parameter
"""
self.length = length
self.amplitude = amplitude
self.sigma = sigma
class DragGaussianWaveform:
"""DRAG (Derivative Removal by Adiabatic Gating) Gaussian waveform."""
def __init__(
self,
length: float,
amplitude: float,
sigma: float,
beta: float
):
"""
Initialize DRAG Gaussian waveform.
Args:
length: Pulse length in seconds
amplitude: Peak amplitude
sigma: Gaussian width parameter
beta: DRAG correction parameter
"""
self.length = length
self.amplitude = amplitude
self.sigma = sigma
self.beta = beta
class ConstantWaveform:
"""Constant amplitude waveform."""
def __init__(self, length: float, amplitude: float):
"""
Initialize constant waveform.
Args:
length: Pulse length in seconds
amplitude: Constant amplitude
"""
self.length = length
self.amplitude = amplitude
class ArbitraryWaveform:
"""Custom arbitrary waveform."""
def __init__(self, amplitudes: list[complex]):
"""
Initialize arbitrary waveform.
Args:
amplitudes: Time-sampled amplitude values
"""
self.amplitudes = amplitudes
self.length = len(amplitudes)
# Pulse programming examples
def create_single_qubit_pulse_gate(qubit_frequency: float, rabi_frequency: float, gate_type: str) -> PulseSequence:
"""
Create pulse sequence for single-qubit gate.
Args:
qubit_frequency: Qubit transition frequency in Hz
rabi_frequency: Rabi frequency for π-pulse in Hz
gate_type: Type of gate ('X', 'Y', 'Z', 'H')
Returns:
PulseSequence: Pulse sequence implementing the gate
"""
sequence = PulseSequence()
# Define hardware components
port = Port("drive_port", dt=1e-9) # 1 ns resolution
frame = Frame("qubit_frame", port, qubit_frequency)
if gate_type == 'X':
# π-pulse around X-axis
pulse_length = 1 / (2 * rabi_frequency) # π-pulse duration
waveform = GaussianWaveform(
length=pulse_length,
amplitude=rabi_frequency * 2 * np.pi,
sigma=pulse_length / 4
)
sequence.play(frame, waveform)
elif gate_type == 'Y':
# π-pulse around Y-axis (π/2 phase shift)
pulse_length = 1 / (2 * rabi_frequency)
sequence.set_phase(frame, np.pi/2)
waveform = GaussianWaveform(
length=pulse_length,
amplitude=rabi_frequency * 2 * np.pi,
sigma=pulse_length / 4
)
sequence.play(frame, waveform)
sequence.set_phase(frame, 0) # Reset phase
elif gate_type == 'H':
# Hadamard via Y(π/2) - X(π) - Y(π/2) decomposition
pulse_length = 1 / (4 * rabi_frequency) # π/2-pulse duration
# First Y(π/2)
sequence.set_phase(frame, np.pi/2)
y_pulse = GaussianWaveform(
length=pulse_length,
amplitude=rabi_frequency * 2 * np.pi,
sigma=pulse_length / 4
)
sequence.play(frame, y_pulse)
# X(π)
sequence.set_phase(frame, 0)
x_pulse = GaussianWaveform(
length=2*pulse_length,
amplitude=rabi_frequency * 2 * np.pi,
sigma=pulse_length / 2
)
sequence.play(frame, x_pulse)
# Final Y(π/2)
sequence.set_phase(frame, np.pi/2)
sequence.play(frame, y_pulse)
sequence.set_phase(frame, 0)
return sequence
def create_two_qubit_cross_resonance_gate(
control_freq: float,
target_freq: float,
cr_amplitude: float
) -> PulseSequence:
"""
Create cross-resonance pulse sequence for two-qubit gate.
Args:
control_freq: Control qubit frequency in Hz
target_freq: Target qubit frequency in Hz
cr_amplitude: Cross-resonance drive amplitude
Returns:
PulseSequence: Cross-resonance gate pulse sequence
"""
sequence = PulseSequence()
# Hardware setup
control_port = Port("control_port", dt=1e-9)
target_port = Port("target_port", dt=1e-9)
control_frame = Frame("control_frame", control_port, control_freq)
target_frame = Frame("target_frame", target_port, target_freq)
# Cross-resonance drive on target frequency via control port
cr_frame = Frame("cr_frame", control_port, target_freq)
# Cross-resonance pulse (flat-top with Gaussian edges)
cr_duration = 320e-9 # 320 ns typical CR gate time
rise_time = 20e-9 # 20 ns rise/fall time
# Rising edge
rise_waveform = GaussianWaveform(
length=rise_time,
amplitude=cr_amplitude,
sigma=rise_time / 4
)
# Flat top
flat_duration = cr_duration - 2 * rise_time
flat_waveform = ConstantWaveform(flat_duration, cr_amplitude)
# Falling edge
fall_waveform = GaussianWaveform(
length=rise_time,
amplitude=-cr_amplitude, # Negative for falling
sigma=rise_time / 4
)
# Play CR pulse sequence
sequence.play(cr_frame, rise_waveform)
sequence.play(cr_frame, flat_waveform)
sequence.play(cr_frame, fall_waveform)
# Echo cancellation pulses on control qubit
echo_pulse = GaussianWaveform(
length=cr_duration,
amplitude=cr_amplitude / 4, # Reduced amplitude
sigma=cr_duration / 8
)
sequence.play(control_frame, echo_pulse)
# Synchronization barrier
sequence.barrier([control_frame, target_frame, cr_frame])
return sequence
def optimize_pulse_fidelity(
target_unitary: np.ndarray,
pulse_parameters: dict,
constraints: dict
) -> dict:
"""
Optimize pulse sequence for maximum gate fidelity.
Args:
target_unitary: Target gate unitary matrix
pulse_parameters: Initial pulse parameter values
constraints: Hardware and physics constraints
Returns:
dict: Optimized pulse parameters and fidelity analysis
"""
optimization_result = {
'optimized_parameters': {},
'achieved_fidelity': 0.0,
'optimization_history': [],
'constraint_violations': {},
'recommendations': []
}
# Extract constraints
max_amplitude = constraints.get('max_amplitude', 1e8) # Hz
min_duration = constraints.get('min_duration', 1e-9) # s
max_duration = constraints.get('max_duration', 1e-6) # s
# Simplified optimization (would use gradient-based methods)
initial_amplitude = pulse_parameters.get('amplitude', max_amplitude / 2)
initial_duration = pulse_parameters.get('duration', 50e-9)
initial_sigma = pulse_parameters.get('sigma', initial_duration / 4)
# Grid search over parameter space (simplified)
best_fidelity = 0.0
best_params = pulse_parameters.copy()
amplitude_range = np.linspace(max_amplitude/10, max_amplitude, 10)
duration_range = np.linspace(min_duration*10, max_duration/10, 10)
for amp in amplitude_range:
for dur in duration_range:
# Simulate gate with these parameters
simulated_fidelity = simulate_pulse_gate_fidelity(
target_unitary, amp, dur, dur/4
)
if simulated_fidelity > best_fidelity:
best_fidelity = simulated_fidelity
best_params = {
'amplitude': amp,
'duration': dur,
'sigma': dur/4
}
optimization_result['optimized_parameters'] = best_params
optimization_result['achieved_fidelity'] = best_fidelity
# Generate recommendations
if best_fidelity < 0.99:
optimization_result['recommendations'].append(
"Consider DRAG correction for improved fidelity"
)
if best_params['duration'] > max_duration / 2:
optimization_result['recommendations'].append(
"Long pulse duration may increase decoherence"
)
return optimization_result
def simulate_pulse_gate_fidelity(target_unitary: np.ndarray, amplitude: float, duration: float, sigma: float) -> float:
"""Simplified pulse gate fidelity simulation."""
# This would involve solving the Schrödinger equation
# For now, return a mock fidelity based on parameter reasonableness
# Assume optimal parameters give ~99% fidelity
optimal_duration = 50e-9 # 50 ns
optimal_amplitude = 1e7 # 10 MHz
duration_factor = 1 - abs(duration - optimal_duration) / optimal_duration
amplitude_factor = 1 - abs(amplitude - optimal_amplitude) / optimal_amplitude
fidelity = 0.95 * duration_factor * amplitude_factor
return max(0.5, min(0.999, fidelity)) # Clamp between 50% and 99.9%from braket.error_mitigation import ErrorMitigation, Debias
class ErrorMitigation:
"""Base error mitigation interface."""
def mitigate(self, task_results: list) -> list:
"""
Apply error mitigation to task results.
Args:
task_results: Raw quantum task results
Returns:
list: Mitigated results
"""
pass
class Debias(ErrorMitigation):
"""Debiasing error mitigation technique."""
def __init__(self, noise_model=None):
"""
Initialize debiasing error mitigation.
Args:
noise_model: Optional noise model for correction
"""
self.noise_model = noise_model
def mitigate(self, task_results: list) -> list:
"""
Apply debiasing to measurement results.
Args:
task_results: Task results to debias
Returns:
list: Debiased results
"""
pass
# Error mitigation examples
def implement_zero_noise_extrapolation(
circuit,
device,
noise_scaling_factors: list[float] = [1.0, 2.0, 3.0]
) -> dict:
"""
Implement zero-noise extrapolation (ZNE) error mitigation.
Args:
circuit: Quantum circuit to execute with error mitigation
device: Quantum device for execution
noise_scaling_factors: Noise scaling factors for extrapolation
Returns:
dict: ZNE results and extrapolated values
"""
zne_results = {
'noise_factors': noise_scaling_factors,
'measured_values': [],
'extrapolated_value': 0.0,
'extrapolation_error': 0.0,
'mitigation_overhead': len(noise_scaling_factors)
}
# Execute circuit at different noise levels
for noise_factor in noise_scaling_factors:
# Create noise-scaled circuit (simplified - would need proper implementation)
scaled_circuit = scale_circuit_noise(circuit, noise_factor)
# Execute and measure expectation value
task = device.run(scaled_circuit, shots=10000)
result = task.result()
if hasattr(result, 'values'):
expectation_value = result.values[0]
else:
# Calculate expectation from measurement counts
expectation_value = calculate_expectation_from_counts(
result.measurement_counts
)
zne_results['measured_values'].append(expectation_value)
# Extrapolate to zero noise
extrapolated_value, error = extrapolate_to_zero_noise(
noise_scaling_factors, zne_results['measured_values']
)
zne_results['extrapolated_value'] = extrapolated_value
zne_results['extrapolation_error'] = error
return zne_results
def implement_readout_error_mitigation(
circuits: list,
device,
calibration_shots: int = 10000
) -> dict:
"""
Implement readout error mitigation using confusion matrix.
Args:
circuits: Circuits to execute with readout error correction
device: Quantum device
calibration_shots: Shots for calibration measurements
Returns:
dict: Results with readout error correction applied
"""
mitigation_results = {
'confusion_matrix': None,
'corrected_results': [],
'improvement_metrics': {}
}
# Step 1: Calibrate readout errors
n_qubits = max(circuit.qubit_count for circuit in circuits)
confusion_matrix = calibrate_readout_errors(device, n_qubits, calibration_shots)
mitigation_results['confusion_matrix'] = confusion_matrix
# Step 2: Execute circuits and apply correction
for circuit in circuits:
# Execute circuit
task = device.run(circuit, shots=10000)
raw_counts = task.result().measurement_counts
# Apply readout error correction
corrected_counts = apply_readout_correction(
raw_counts, confusion_matrix
)
mitigation_results['corrected_results'].append({
'circuit_index': len(mitigation_results['corrected_results']),
'raw_counts': raw_counts,
'corrected_counts': corrected_counts
})
# Calculate improvement metrics
mitigation_results['improvement_metrics'] = calculate_mitigation_improvement(
mitigation_results['corrected_results']
)
return mitigation_results
def implement_virtual_distillation(
circuit,
device,
num_copies: int = 5,
shots_per_copy: int = 2000
) -> dict:
"""
Implement virtual distillation error mitigation.
Args:
circuit: Circuit to execute with virtual distillation
device: Quantum device
num_copies: Number of virtual copies
shots_per_copy: Shots per copy
Returns:
dict: Virtual distillation results
"""
vd_results = {
'num_copies': num_copies,
'copy_results': [],
'distilled_result': 0.0,
'variance_reduction': 0.0
}
copy_values = []
# Execute multiple copies of the circuit
for copy_idx in range(num_copies):
task = device.run(circuit, shots=shots_per_copy)
result = task.result()
# Calculate expectation value for this copy
if hasattr(result, 'values'):
expectation = result.values[0]
else:
expectation = calculate_expectation_from_counts(result.measurement_counts)
copy_values.append(expectation)
vd_results['copy_results'].append({
'copy_index': copy_idx,
'expectation_value': expectation,
'measurement_counts': result.measurement_counts
})
# Apply virtual distillation formula
# For odd number of copies: median
# For even number: could use other combining strategies
if num_copies % 2 == 1:
distilled_value = np.median(copy_values)
else:
# Use weighted average with outlier removal
copy_array = np.array(copy_values)
q1, q3 = np.percentile(copy_array, [25, 75])
iqr = q3 - q1
lower_bound = q1 - 1.5 * iqr
upper_bound = q3 + 1.5 * iqr
# Filter outliers and average
filtered_values = copy_array[
(copy_array >= lower_bound) & (copy_array <= upper_bound)
]
distilled_value = np.mean(filtered_values) if len(filtered_values) > 0 else np.mean(copy_array)
vd_results['distilled_result'] = distilled_value
# Calculate variance reduction
raw_variance = np.var(copy_values)
# Virtual distillation typically reduces variance by ~1/sqrt(N)
expected_variance_reduction = 1 / np.sqrt(num_copies)
vd_results['variance_reduction'] = expected_variance_reduction
return vd_results
def scale_circuit_noise(circuit, noise_factor: float):
"""Scale noise in quantum circuit (simplified implementation)."""
# This would involve adding noise gates or modifying existing noise
# For now, return original circuit (real implementation would add noise)
return circuit
def extrapolate_to_zero_noise(noise_factors: list[float], measured_values: list[float]) -> tuple[float, float]:
"""Extrapolate measured values to zero noise using polynomial fit."""
# Linear extrapolation (could use higher-order polynomials)
coeffs = np.polyfit(noise_factors, measured_values, deg=1)
# Extrapolate to zero noise (x=0)
extrapolated_value = coeffs[1] # y-intercept
# Estimate error from fit quality
fit_values = np.polyval(coeffs, noise_factors)
fit_error = np.sqrt(np.mean((np.array(measured_values) - fit_values)**2))
return float(extrapolated_value), float(fit_error)
def calibrate_readout_errors(device, n_qubits: int, shots: int) -> np.ndarray:
"""Calibrate readout error confusion matrix."""
from braket.circuits import Circuit
confusion_matrix = np.zeros((2**n_qubits, 2**n_qubits))
# Measure each computational basis state
for state_idx in range(2**n_qubits):
# Prepare computational basis state |state_idx⟩
prep_circuit = Circuit()
# Convert state index to binary and apply X gates
binary_state = format(state_idx, f'0{n_qubits}b')
for qubit, bit in enumerate(binary_state):
if bit == '1':
prep_circuit.x(qubit)
# Measure
prep_circuit.measure_all()
# Execute calibration measurement
task = device.run(prep_circuit, shots=shots)
counts = task.result().measurement_counts
# Fill confusion matrix row
for measured_state, count in counts.items():
measured_idx = int(measured_state, 2)
confusion_matrix[state_idx, measured_idx] = count / shots
return confusion_matrix
def apply_readout_correction(raw_counts: dict, confusion_matrix: np.ndarray) -> dict:
"""Apply readout error correction using confusion matrix inversion."""
# Convert counts to probability vector
total_shots = sum(raw_counts.values())
n_states = len(confusion_matrix)
measured_probs = np.zeros(n_states)
for bitstring, count in raw_counts.items():
state_idx = int(bitstring, 2)
measured_probs[state_idx] = count / total_shots
# Invert confusion matrix to get corrected probabilities
try:
inv_confusion = np.linalg.inv(confusion_matrix)
corrected_probs = inv_confusion @ measured_probs
# Ensure probabilities are non-negative (physical constraint)
corrected_probs = np.maximum(corrected_probs, 0)
corrected_probs /= np.sum(corrected_probs) # Renormalize
except np.linalg.LinAlgError:
# If matrix is singular, use pseudo-inverse
inv_confusion = np.linalg.pinv(confusion_matrix)
corrected_probs = inv_confusion @ measured_probs
corrected_probs = np.maximum(corrected_probs, 0)
corrected_probs /= np.sum(corrected_probs)
# Convert back to counts
corrected_counts = {}
for state_idx, prob in enumerate(corrected_probs):
if prob > 0:
bitstring = format(state_idx, f'0{int(np.log2(n_states))}b')
corrected_counts[bitstring] = int(prob * total_shots)
return corrected_counts
def calculate_expectation_from_counts(counts: dict) -> float:
"""Calculate expectation value ⟨Z⟩ from measurement counts."""
total_shots = sum(counts.values())
expectation = 0.0
for bitstring, count in counts.items():
# Calculate parity (even=+1, odd=-1)
parity = (-1) ** sum(int(bit) for bit in bitstring)
expectation += parity * count / total_shots
return expectationfrom braket.experimental_capabilities import EnableExperimentalCapability
class EnableExperimentalCapability:
"""Context manager for experimental features."""
def __init__(self, capability_name: str):
"""
Initialize experimental capability context.
Args:
capability_name: Name of experimental capability to enable
"""
self.capability_name = capability_name
def __enter__(self) -> 'EnableExperimentalCapability':
"""Enable experimental capability."""
return self
def __exit__(self, exc_type, exc_val, exc_tb) -> None:
"""Disable experimental capability."""
pass
# Experimental features examples
def use_experimental_classical_control():
"""Example of using experimental classical control features."""
with EnableExperimentalCapability("classical_control"):
# Access experimental classical control capabilities
from braket.experimental_capabilities import classical_control
# This would enable features like:
# - Mid-circuit measurements with classical feedback
# - Conditional quantum operations
# - Real-time classical processing during quantum execution
experimental_features = {
'mid_circuit_measurement': True,
'classical_feedback': True,
'conditional_gates': True,
'real_time_processing': True
}
return experimental_features
def explore_advanced_noise_modeling():
"""Explore experimental advanced noise modeling capabilities."""
with EnableExperimentalCapability("advanced_noise"):
# Access experimental noise modeling features
experimental_noise_features = {
'correlated_noise': 'Multi-qubit correlated noise channels',
'time_dependent_noise': 'Time-varying noise parameters',
'device_specific_noise': 'Hardware-calibrated noise models',
'non_markovian_effects': 'Memory effects in noise evolution'
}
return experimental_noise_features
def demonstrate_experimental_optimization():
"""Demonstrate experimental optimization capabilities."""
with EnableExperimentalCapability("advanced_optimization"):
optimization_features = {
'adaptive_shot_allocation': 'Dynamic shot count optimization',
'circuit_cutting': 'Large circuit decomposition',
'error_extrapolation': 'Advanced error extrapolation methods',
'hardware_aware_compilation': 'Device-specific circuit optimization'
}
# Example: Adaptive shot allocation
def adaptive_shot_optimization(circuits: list, target_accuracy: float) -> dict:
"""
Experimental adaptive shot allocation for circuit collection.
Args:
circuits: Circuits requiring optimization
target_accuracy: Target measurement accuracy
Returns:
dict: Optimized shot allocation strategy
"""
shot_allocation = {}
for i, circuit in enumerate(circuits):
# Estimate required shots based on circuit properties
estimated_variance = estimate_measurement_variance(circuit)
required_shots = int(estimated_variance / (target_accuracy**2))
# Apply experimental optimization heuristics
if circuit.depth > 50:
required_shots *= 2 # Deeper circuits need more shots
if has_small_angle_rotations(circuit):
required_shots *= 1.5 # Small angles need higher precision
shot_allocation[f'circuit_{i}'] = {
'required_shots': required_shots,
'estimated_variance': estimated_variance,
'optimization_factor': required_shots / 1000 # Compared to baseline
}
return shot_allocation
return {
'features': optimization_features,
'adaptive_optimizer': adaptive_shot_optimization
}
def estimate_measurement_variance(circuit) -> float:
"""Estimate measurement variance for shot optimization."""
# Simplified variance estimation based on circuit properties
base_variance = 0.25 # Maximum variance for uniform distribution
# Adjust based on circuit depth (deeper = more noise = higher variance)
depth_factor = min(2.0, 1 + circuit.depth / 100)
# Adjust based on number of measured qubits
qubit_factor = circuit.qubit_count / 10
return base_variance * depth_factor * qubit_factor
def has_small_angle_rotations(circuit) -> bool:
"""Check if circuit contains small-angle rotations requiring high precision."""
small_angle_threshold = 0.1 # radians
for instruction in circuit.instructions:
gate = instruction.operator
if hasattr(gate, 'angle'):
if abs(gate.angle) < small_angle_threshold:
return True
return False
def demonstrate_quantum_error_correction_experiments():
"""Demonstrate experimental quantum error correction capabilities."""
with EnableExperimentalCapability("quantum_error_correction"):
qec_experiments = {
'surface_codes': {
'description': 'Surface code implementation and testing',
'min_qubits': 17, # Smallest logical qubit
'features': ['syndrome extraction', 'logical operations', 'error correction']
},
'color_codes': {
'description': 'Color code quantum error correction',
'min_qubits': 7, # 7-qubit color code
'features': ['triangular lattice', 'transversal gates', 'fault tolerance']
},
'repetition_codes': {
'description': 'Simple repetition codes for bit-flip errors',
'min_qubits': 3, # 3-qubit repetition code
'features': ['bit flip correction', 'syndrome measurement', 'majority voting']
}
}
def create_simple_qec_circuit(code_type: str = 'repetition') -> dict:
"""Create simple quantum error correction demonstration circuit."""
from braket.circuits import Circuit
if code_type == 'repetition':
# 3-qubit bit-flip repetition code
circuit = Circuit()
# Encode logical |0⟩ or |1⟩
# |0⟩_L = |000⟩, |1⟩_L = |111⟩
# For |+⟩_L state: (|000⟩ + |111⟩)/√2
circuit.h(0) # Create superposition on first qubit
circuit.cnot(0, 1) # Entangle with second qubit
circuit.cnot(0, 2) # Entangle with third qubit
# Syndrome measurement (detect single bit-flip errors)
circuit.cnot(0, 3) # Ancilla 3: measures X₀X₁
circuit.cnot(1, 3)
circuit.cnot(1, 4) # Ancilla 4: measures X₁X₂
circuit.cnot(2, 4)
# Measure syndrome qubits
circuit.measure([3, 4])
qec_info = {
'circuit': circuit,
'logical_qubits': 1,
'physical_qubits': 3,
'ancilla_qubits': 2,
'correctable_errors': ['single bit flip'],
'code_distance': 3
}
return qec_info
return {
'available_codes': qec_experiments,
'circuit_generator': create_simple_qec_circuit
}from braket.emulation import Emulator, PassManager
class Emulator:
"""Quantum circuit emulator with compilation passes."""
def __init__(
self,
pass_manager: PassManager = None,
target_device = None
):
"""
Initialize quantum circuit emulator.
Args:
pass_manager: Compilation pass manager
target_device: Target device for emulation properties
"""
self.pass_manager = pass_manager or PassManager()
self.target_device = target_device
def emulate(
self,
circuit,
shots: int = 1000,
inputs: dict = None
):
"""
Emulate quantum circuit with compilation.
Args:
circuit: Quantum circuit to emulate
shots: Number of measurement shots
inputs: Input parameters for parameterized circuits
Returns:
EmulationResult: Emulation results with compilation info
"""
pass
def add_pass(self, pass_instance) -> 'Emulator':
"""
Add compilation pass to emulator.
Args:
pass_instance: Compilation pass to add
Returns:
Emulator: Self for method chaining
"""
self.pass_manager.add_pass(pass_instance)
return self
class PassManager:
"""Compilation pass management for quantum circuits."""
def __init__(self):
"""Initialize empty pass manager."""
self.passes = []
def add_pass(self, pass_instance) -> 'PassManager':
"""
Add compilation pass.
Args:
pass_instance: Pass to add
Returns:
PassManager: Self for method chaining
"""
self.passes.append(pass_instance)
return self
def run(self, circuit):
"""
Run all passes on circuit.
Args:
circuit: Input quantum circuit
Returns:
Circuit: Compiled quantum circuit
"""
compiled_circuit = circuit
for pass_instance in self.passes:
compiled_circuit = pass_instance.run(compiled_circuit)
return compiled_circuit
# Emulation examples
def create_optimized_emulator() -> Emulator:
"""
Create emulator with standard optimization passes.
Returns:
Emulator: Configured emulator with optimization
"""
pass_manager = PassManager()
# Add standard optimization passes
# Note: Actual pass implementations would be more complex
# pass_manager.add_pass(GateCommutationPass())
# pass_manager.add_pass(RedundantGateEliminationPass())
# pass_manager.add_pass(CircuitDepthOptimizationPass())
emulator = Emulator(pass_manager=pass_manager)
return emulator
def benchmark_emulation_performance(circuit) -> dict:
"""
Benchmark emulation vs direct simulation performance.
Args:
circuit: Circuit to benchmark
Returns:
dict: Performance comparison results
"""
import time
from braket.devices import LocalSimulator
benchmark_results = {
'circuit_info': {
'qubit_count': circuit.qubit_count,
'depth': circuit.depth,
'gate_count': len(circuit.instructions)
},
'simulation': {},
'emulation': {}
}
# Direct simulation
simulator = LocalSimulator()
start_time = time.time()
sim_task = simulator.run(circuit, shots=1000)
sim_result = sim_task.result()
sim_time = time.time() - start_time
benchmark_results['simulation'] = {
'execution_time': sim_time,
'compilation_time': 0,
'result_counts': sim_result.measurement_counts
}
# Emulation with compilation
emulator = create_optimized_emulator()
start_time = time.time()
compile_start = time.time()
compiled_circuit = emulator.pass_manager.run(circuit)
compile_time = time.time() - compile_start
emu_result = emulator.emulate(compiled_circuit, shots=1000)
total_emu_time = time.time() - start_time
benchmark_results['emulation'] = {
'execution_time': total_emu_time,
'compilation_time': compile_time,
'optimizations_applied': len(emulator.pass_manager.passes),
'compiled_circuit_depth': compiled_circuit.depth if hasattr(compiled_circuit, 'depth') else 'Unknown'
}
# Performance analysis
benchmark_results['analysis'] = {
'speedup_factor': sim_time / total_emu_time if total_emu_time > 0 else float('inf'),
'compilation_overhead': compile_time / total_emu_time if total_emu_time > 0 else 0,
'depth_reduction': (circuit.depth - (compiled_circuit.depth if hasattr(compiled_circuit, 'depth') else circuit.depth)) / circuit.depth if circuit.depth > 0 else 0
}
return benchmark_resultsfrom braket.experimental_capabilities import EnableExperimentalCapability
class EnableExperimentalCapability:
"""Context manager for enabling experimental features."""
def __init__(self, capability_name: str):
"""
Initialize experimental capability context.
Args:
capability_name: Name of experimental capability to enable
"""
self.capability_name = capability_name
def __enter__(self):
"""Enter experimental capability context."""
pass
def __exit__(self, exc_type, exc_val, exc_tb):
"""Exit experimental capability context."""
pass
# Experimental capabilities examples
def access_experimental_features() -> dict:
"""
Demonstrate access to experimental quantum computing features.
Returns:
dict: Available experimental capabilities
"""
experimental_features = {
'available_capabilities': [
'classical_control',
'adaptive_circuits',
'real_time_feedback',
'advanced_error_correction',
'novel_gate_sets'
],
'usage_examples': {},
'stability_warnings': {
'api_stability': 'Experimental APIs may change without notice',
'result_reliability': 'Results may vary between SDK versions',
'production_readiness': 'Not recommended for production use'
}
}
# Classical control example (IQM-specific)
def classical_control_example():
"""Demonstrate classical control features."""
try:
with EnableExperimentalCapability('classical_control'):
from braket.experimental_capabilities.iqm import classical_control
# This would enable classical control features
# Actual implementation depends on device support
control_config = {
'conditional_gates': True,
'real_time_feedback': True,
'adaptive_measurements': True
}
return {
'status': 'enabled',
'configuration': control_config,
'supported_devices': ['IQM Adonis', 'IQM Apollo']
}
except Exception as e:
return {
'status': 'unavailable',
'error': str(e),
'reason': 'Experimental feature not available in current environment'
}
experimental_features['usage_examples']['classical_control'] = classical_control_example()
# Advanced error correction
def advanced_error_correction_example():
"""Demonstrate advanced error correction features."""
with EnableExperimentalCapability('advanced_error_correction'):
# Experimental error correction protocols
advanced_qec = {
'surface_codes': {
'supported': True,
'min_qubits': 17, # Smallest surface code
'features': ['arbitrary distance', 'custom boundary conditions']
},
'color_codes': {
'supported': True,
'min_qubits': 15, # Color code triangle
'features': ['higher threshold', 'transversal gates']
},
'topological_codes': {
'supported': False,
'reason': 'Requires specific hardware topology'
}
}
return advanced_qec
experimental_features['usage_examples']['advanced_error_correction'] = advanced_error_correction_example()
return experimental_features
def create_experimental_workflow() -> dict:
"""
Create experimental quantum computing workflow.
Returns:
dict: Experimental workflow configuration
"""
workflow = {
'stages': [
'feature_detection',
'capability_enablement',
'experimental_execution',
'result_validation',
'fallback_handling'
],
'implementation': {}
}
def feature_detection_stage():
"""Detect available experimental features."""
available_features = []
# Check for classical control
try:
with EnableExperimentalCapability('classical_control'):
available_features.append('classical_control')
except:
pass
# Check for advanced error correction
try:
with EnableExperimentalCapability('advanced_error_correction'):
available_features.append('advanced_error_correction')
except:
pass
return {
'detected_features': available_features,
'detection_method': 'capability_probing',
'confidence': 'high' if available_features else 'low'
}
def experimental_execution_stage(circuit, experimental_config: dict):
"""Execute circuit with experimental features."""
execution_plan = {
'base_circuit': circuit,
'experimental_modifications': [],
'fallback_strategy': 'standard_execution'
}
# Apply experimental modifications based on config
if 'classical_control' in experimental_config.get('enabled_features', []):
execution_plan['experimental_modifications'].append({
'type': 'classical_control',
'description': 'Enable conditional gate execution',
'impact': 'Allows adaptive circuit behavior'
})
if 'advanced_error_correction' in experimental_config.get('enabled_features', []):
execution_plan['experimental_modifications'].append({
'type': 'advanced_qec',
'description': 'Apply experimental error correction',
'impact': 'Improved fidelity with overhead'
})
return execution_plan
workflow['implementation'] = {
'feature_detection': feature_detection_stage,
'experimental_execution': experimental_execution_stage
}
return workflowThis comprehensive advanced features documentation covers all the sophisticated quantum computing capabilities provided by the Amazon Braket SDK, including analog Hamiltonian simulation, quantum annealing, pulse-level control, error mitigation techniques, circuit emulation infrastructure, and experimental features for cutting-edge quantum computing research and development.
Install with Tessl CLI
npx tessl i tessl/pypi-amazon-braket-sdk