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# Solving MaxCut with Mitiq-improved QAOA
+++
In this notebook we solve a simple [_MaxCut_ problem](https://en.wikipedia.org/wiki/Maximum_cut) with the
_Quantum Approximate Optimization Algorithm_ (QAOA) {cite}`Farhi_2014_arXiv` executed on a simulated noisy backend.
In particular we are interested in investigating how Mitiq can help reduce errors and improve the results.
+++
## The MaxCut problem
+++
A **graph** is a mathematical object characterized by a set $V$ of **vertices (or nodes)** that we can
enumerate with integers $V=\{0, 1, 2, \dots, n-1\}$ and a set $E$ of **edges** (pairs of nodes) which can be defined as
$E=\{(a_1, b_1), (a_2, b_2), ...., (a_m, b_m)\}$, where $a_j\neq b_j$ and $a_j, b_j \in V$.
**Note:** If we are not interested in isolated nodes (not connected to any edge), the set of edges $E$ completely
determine the graph $G=(V, E)$.
Therefore, in Python, we can represent a graph without isolated nodes as a **list of tuples**, where each
tuple is a **pair of integers**. For example a **square graph** can be expressed as:
```{code-cell} ipython3
# Square graph
square_graph = [(0, 1), (1, 2), (2, 3), (3, 0)]
```
Given a graph $(V, E)$, the **MaxCut problem** is to divide the nodes $V$ into two disjoint subsets
$V_A$ and $V_B$, such that the number of cuts (edges with one vertex in $V_A$ and one vertex in $V_B$) is maximized.
```{code-cell} ipython3
from typing import List, Tuple
def count_cuts(graph: List[Tuple[int]], set_a: set, set_b: set):
"""Counts the number of cuts of a graph bipartition."""
num_cuts = 0
for edge in graph:
if edge[0] in set_a and edge[1] in set_b:
num_cuts += 1
if edge[0] in set_b and edge[1] in set_a:
num_cuts += 1
return num_cuts
```
For example, for the square graph previously defined, the maximum number of cuts is $4$ which can be
achieved by multiple solutions. For example one of the two optimal solutions is:
```{code-cell} ipython3
set_a = {0, 2}
set_b = {1, 3}
```
Indeed, in this case, we have a cut for all the edges of `square_graph`, and so their number is maximum.
```{code-cell} ipython3
count_cuts(square_graph, set_a, set_b)
```
An example of a sub-optimal solution is instead:
```{code-cell} ipython3
set_a = {0}
set_b = {1, 2, 3}
count_cuts(square_graph, set_a, set_b)
```
### Representing a solution as bitstring
+++
A handy way of representing a candidate solution of the MaxCut problem, is to use a bitstring $s_n \cdots s_2s_1$
in which each bit $s_j$ is associated to the $j_{\rm th}$ node of the graph. The value of each bit, $0$ or $1$,
can be used to represent the corresponding subset, $V_A$ or $V_B$, to which the node belongs.
For example, using a big-endian convention, the previous optimal and sub-optimal solutions can be represented as:
```{code-cell} ipython3
optimal_string = "1010"
sub_optimal_string = "1110"
```
The corresponding function to count the number of graph cuts can be written in the following way wich is very
similar to the quantum cost function that we will define in the next section.
```{code-cell} ipython3
def count_cuts_from_string(graph: List[Tuple[int]], bitstring: str):
"""Counts the number of cuts of a graph bipartition represented as a (big-endian) bitstring.
"""
cost = 0
for i, j in graph:
z1 = (2 * int(bitstring[-i]) - 1)
z2 = (2 * int(bitstring[-j]) - 1)
cost += -(1 - z1 * z2) // 2
return -cost
```
Let's test this function:
```{code-cell} ipython3
# Test the function
count_cuts_from_string(square_graph, optimal_string)
```
```{code-cell} ipython3
count_cuts_from_string(square_graph, sub_optimal_string)
```
The MaxCut problem is **NP-hard**. This means that it is computationally very hard (at least as hard
as any NP problem). It is widely suspected that NP-hard problems will never admit a polynomial algorithm
even if we had at disposal an ideal quantum computer.
However, for practical applications, it is often possible to obtain good **approximations** of the
optimal exact solution. In this notebook we are interested in using the _Quantum Approximate Optimization
Algorithm_ (QAOA) to get an approximate solution the MaxCut problem for a given graph.
+++
## Embedding a MaxCut problem into a physical Hamiltonian
+++
Given a graph $G=(V,E)$ with $n=|V|$ nodes and $m=|E|$ edges, one can define the following Hamiltonian
acting on a system of $n$ qubits:
$$H = \sum_{(i,\, j) \in E} \frac{1}{2} (1 - Z_i Z_j),$$
where $Z_k$ is the Pauli-Z operator applied to the qubit $k$, such that $Z_k | 0 \rangle_k = +| 0 \rangle_k$ and $Z_k | 1 \rangle_k = - |1 \rangle_k$.
Now we can associate each qubit of the system to a vertex of the graph. A potential solution of the MaxCut
problem (i.e., the partition $(V_A, V_B)$) can be represented by a quantum product state:
$$|\psi \rangle = |s_n \rangle \cdots |s_2 \rangle |s_1\rangle, $$
where $s_j=0$ if $j \in V_A$, while $s_j=1$ if $j \in V_B$.
In this case it is easy to check that the corresponding number of cuts is given by the opposite of the
expectation value of the Hamiltonian $H$:
$$ \text{number of cuts } = - \langle \psi | H | \psi \rangle .$$
In this physical picture, the MaxCut problem corresponds to the problem of finding the ground state of $H$
and the maximum number of cuts is equal to minus the ground state energy.
+++
### Define the QAOA cost Hamiltonian using Cirq
```{code-cell} ipython3
from cirq import NamedQubit, Circuit, identity_each, ZZ
import numpy as np
def qaoa_hamiltonian(graph: List[Tuple[float]]) -> np.ndarray:
"""Returns the cost Hamiltonian associated to the input graph.
"""
# Get all the nodes of the graph
nodes = list({node for edge in graph for node in edge})
# Initialize the qubits. One for each node.
qreg = [NamedQubit(str(nn)) for nn in nodes]
# Define the Hamiltonian as a NumPy array
np_identity = np.eye(2 ** len(nodes))
zz_terms = np.real([Circuit([identity_each(*qreg), ZZ(qreg[i], qreg[j])]).unitary() for i, j in graph])
local_terms = [-0.5 * (np_identity - zz_term) for zz_term in zz_terms]
return sum(local_terms)
```
Since it is diagonal in the computational basis, we can get the ground state energy as follows:
```{code-cell} ipython3
eig_vals = np.diag(qaoa_hamiltonian(square_graph))
# Ground state energy
min(eig_vals)
```
which, as expected, corresponds to the opposite of the maximum number of cuts of the original graph.
The associated optimal eigenstates are:
```{code-cell} ipython3
nodes = list({node for edge in square_graph for node in edge})
num_nodes = len(nodes)
optimal_bitstrings = [f"{j:b}".zfill(num_nodes) for j, eig_val in enumerate(eig_vals) if eig_val == min(eig_vals)]
optimal_bitstrings
```
Which indeed correspond to the 2 optimal bipartitions of the original MaxCut problem:
```{code-cell} ipython3
[count_cuts_from_string(square_graph, bitstring) for bitstring in optimal_bitstrings]
```
## Using the Quantum Approximate Optimization Algorithm to find the ground state
+++
The size of the previously introduced Hamiltonian is $2^n \times 2^n$. So, when the graph has many nodes,
finding the eigenvalues and or the eigenstates as we did above becomes exponentially hard.
```{admonition} Question
:class: attention
Is there a way of finding the ground state of a Hamiltonian using a near-term quantum computer?
```
This is where Quantum Approximate Optimization Algorithm (QAOA) {cite}`Farhi_2014_arXiv` comes into play.
This method consists of generating a potential solution state through a variational circuit
$U_{\vec \alpha, \vec \beta}$ which depends on two vectors of $p$ real parameters
$\vec \alpha = (\alpha_1, .... \alpha_p)$, $\vec \beta= (\beta_1, .... \beta_p)$ and has the following structure:
$$|\psi(\vec \alpha, \vec \beta) \rangle = U_{\vec \alpha, \vec \beta}|+\rangle^{\otimes n} = R_{\alpha_p} W_{\beta_p} \cdots R_{\alpha_1} W_{\beta_1} |+\rangle^{\otimes n},$$
where $| + \rangle = (|0\rangle + |1\rangle)/\sqrt{2}$ and
$$W_{\beta} = e^{i \beta H }, \quad R_{\alpha} = e^{i \alpha \sum_{j=1}^n X_j },$$
corresponding to the time evolution generated by the system Hamiltonian $H$ and by a mixing Hamiltonian
$H_{\rm mix}= \sum_j X_j$, respectively.
After applying the circuit to generate $|\psi(\vec \alpha, \vec \beta) \rangle$, one can easily measure
the energy of the final state
$$E(\vec \alpha, \vec \beta) = \langle \psi(\vec \alpha, \vec \beta) | H |\psi(\vec \alpha, \vec \beta)\rangle,$$
via simple measurements in the computational basis of the qubits. Repeating this procedure over many
steps and minimizing the **cost function** $E(\vec \alpha, \vec \beta)$ with respect to the parameters
$\vec \alpha$ and $\vec \beta$ one can approximate the ground state of $H$.
The maximum number of cuts for the original graph will be given by the opposite of the optimal cost: $- \min[ E(\vec \alpha, \vec \beta)]$.
The corresponding state will be a superposition of one or more optimal solution states
$|s_1 \rangle |s_2 \rangle \cdots |s_n\rangle$ representing optimal bipartitions $(V_A, V_B)$ of the MaxCut problem.
+++
### Defining the QAOA ansatz
```{code-cell} ipython3
from cirq import H, X
from typing import List, Tuple
def qaoa_ansatz(graph: List[Tuple[float]], params: List[float]) -> Circuit:
"""Generates a QAOA circuit associated to the input graph, for
a specific choice of variational parameters.
Args:
graph: The input graph.
params: The variational parameters.
Returns:
The QAOA circuit.
"""
# Get the list of unique nodes from the list of edges
nodes = list({node for edge in graph for node in edge})
# Initialize the qubits
qreg = [NamedQubit(str(nn)) for nn in nodes]
# Define the Hamiltonian evolution (up to an additive and a multiplicative constant)
def h_step(beta: float) -> Circuit:
return Circuit(ZZ(qreg[u], qreg[v]) ** (beta) for u, v in graph)
# Define the mixing evolution (up to an additive and a multiplicative constant)
def mix_step(gamma: float) -> Circuit:
return Circuit(X(qq) ** gamma for qq in qreg)
# State preparation layer
circ = Circuit(H.on_each(qreg))
# Apply QAOA steps
num_steps = len(params) // 2
betas, alphas = params[:num_steps], params[num_steps:]
for beta, alpha in zip(betas, alphas):
circ.append([h_step(beta) + mix_step(alpha)])
return circ
```
For example, a 2-step QAOA circuit can be generated as follows:
```{code-cell} ipython3
betas = [0.1, 0.2]
alphas = [0.3, 0.4]
params = betas + alphas
qaoa_ansatz(square_graph, params)
```
### Defining an "executor" function to run or simulate the experiment
QAOA requires the evaluation of quantum expectation values. Therefore, we define a function which inputs
a generic circuit and returns the expectation value of a generic observable.
```{code-cell} ipython3
from cirq import depolarize, DensityMatrixSimulator
def executor(circ: Circuit, obs: np.array, noise: float) -> float:
"""Simulates a circuit with depolarizing noise at level 'noise' and returns the
expectation value of the observable 'obs'.
"""
SIMULATOR = DensityMatrixSimulator()
# Add the noise
noisy_circ = circ.with_noise(depolarize(p=noise))
# Get the final quantum state
rho = SIMULATOR.simulate(noisy_circ).final_density_matrix
# Return the expectation value
return np.real(np.trace(rho @ obs))
```
For example, let us get the expectation value of the cost Hamiltonian (without optimizing the circuit):
```{code-cell} ipython3
betas = [0.1, 0.2]
alphas = [0.3, 0.4]
params = betas + alphas
circuit = qaoa_ansatz(square_graph, params)
hamiltonian = qaoa_hamiltonian(square_graph)
executor(circuit, obs=hamiltonian, noise=0)
```
### Minimization of the QAOA cost
Let us define a function which can be used for running the QAOA optimization.
```{code-cell} ipython3
from typing import Callable
from scipy.optimize import minimize
def minimize_cost(
cost_function: Callable[[np.array], float],
init_params: np.array,
) -> Tuple[float, np.ndarray, List[float]]:
"""Minimizes a cost function which depends on an array variational parameters.
Args:
cost_function: The cost function to minimize.
init_params: The initial variational parameters.
Returns:
A triple of the minimum cost, the optimal parameters and a list of costs at each iteration steps.
"""
# store the optimization trajectory
traj = []
def callback(xk: np.ndarray) -> bool:
traj.append(cost_function(xk))
return True
results = minimize(
cost_function,
x0=init_params,
method="Nelder-Mead",
callback=callback,
options={"disp": True, "maxiter": 300},
# Set tol=0 to enforce a fixed number of iterations.
# Comment tol=0 to speedup the notebook execution.
tol=0,
)
plt.title("Optimization history")
plt.xlabel("Iteration Step")
plt.ylabel("Cost")
plt.plot(traj)
plt.show()
return results.fun, results.x, traj
```
## Comparing ideal, noisy and mitigated backends
+++
### Ideal simulation
+++
We focus on the square graph and try to solve the associated QAOA algorithm.
First, we consider the ideal situation of a noiseless backend.
```{code-cell} ipython3
from matplotlib import pyplot as plt
graph = [(0, 1), (1, 2), (2, 3), (3, 0)]
betas = [0.0, 0.5]
gammas = [0.7, 1.0]
init_params = betas + gammas
```
```{code-cell} ipython3
def qaoa_ideal_cost(params: np.array) -> float:
"""Ideal cost function of the QAOA problem without noise."""
qaoa_circuit = qaoa_ansatz(graph, params)
qaoa_obs = qaoa_hamiltonian(graph)
return executor(qaoa_circuit, qaoa_obs, noise=0)
ideal_opt_cost, ideal_opt_params, traj = minimize_cost(qaoa_ideal_cost, init_params)
print("Ideal cost: ", np.round(ideal_opt_cost, 4))
```
Since the simulation is exact, we reach the optimal cost associated to (minus) the maximum number of cuts of the graph.
+++
### Using a noisy unmitigated simulator
We assume to have some depolarizing noise. This means that we need to re-define the QAOA cost function using a noisy executor function.
```{code-cell} ipython3
BASE_NOISE = 0.03
def qaoa_noisy_cost(params: np.array) -> float:
"""Noisy cost function of the QAOA problem."""
qaoa_circuit = qaoa_ansatz(graph, params)
qaoa_obs = qaoa_hamiltonian(graph)
return executor(qaoa_circuit, qaoa_obs, noise=BASE_NOISE)
noisy_opt_cost, noisy_opt_params, noisy_traj = minimize_cost(qaoa_noisy_cost, init_params)
```
Because of noise, the QAOA optimization is not able to converge to the optimal solution.
Indeed the variational parameters optimized with noise do not minimize the ideal cost.
```{code-cell} ipython3
print("Noisy cost: ", np.round(noisy_opt_cost, 4))
print("Ideal cost evaluated at noisy parameters: ", np.round(qaoa_ideal_cost(noisy_opt_params), 4))
print("Ideal cost: ", np.round(ideal_opt_cost, 4))
```
### Using a noisy simulator mitigated with Mitiq
Now let's try to mitigate this noise using Mitiq.
This can be done by simply wrapping the noisy executor into a mitigated executor. We will use global folding and a linear inference (using a {class}`.LinearFactory` object) to implement zero-noise extrapolation.
```{code-cell} ipython3
import mitiq
from mitiq.zne import mitigate_executor
from functools import partial
# Choose a noise scaling method
scaling_method = mitiq.zne.scaling.fold_global
# Initialize an inference method (i.e. a Mitiq Factory)
inference_factory = mitiq.zne.inference.LinearFactory(scale_factors=[1.0, 3.0])
# Define the cost function
def qaoa_mitigated_cost(params: np.array) -> float:
"""Cost function of the QAOA problem using error mitigation."""
qaoa_circuit = qaoa_ansatz(graph, params)
qaoa_obs = qaoa_hamiltonian(graph)
noisy_executor = partial(executor, obs=qaoa_obs, noise=BASE_NOISE)
mitigated_executor = mitigate_executor(noisy_executor, factory=inference_factory, scale_noise=scaling_method)
return mitigated_executor(qaoa_circuit)
# Minimize the cost function
mitig_opt_cost, mitig_opt_params, mitig_traj = minimize_cost(qaoa_mitigated_cost, init_params)
```
```{code-cell} ipython3
print("Mitigated cost: ", np.round(mitig_opt_cost, 4))
print("Noisy cost evaluated at noisy parameters: ", np.round(noisy_opt_cost, 4))
print("Noisy cost evaluated at mitigated parameters: ",np.round(qaoa_noisy_cost(mitig_opt_params), 4))
print("Ideal cost evaluated at noisy parameters: ", np.round(qaoa_ideal_cost(noisy_opt_params), 4))
print("Ideal cost evaluated at mitigated parameters: ", np.round(qaoa_ideal_cost(mitig_opt_params), 4))
print("Ideal cost: ", np.round(ideal_opt_cost, 4))
```
:::{note}
The results are clearly enhanced by the application of zero-noise extrapolation.
However the execution time is increased too.
The practical advantage of any error mitigation methods always depends on the trade-off between
the accuracy of the results and the execution time.
:::
+++
## References
- Edward Farhi, Jeffrey Goldstone, Sam Gutmann, _A Quantum Approximate Optimization Algorithm_, {cite}`Farhi_2014_arXiv`
- [MaxCut tutorial in PennyLane](https://pennylane.ai/qml/demos/tutorial_qaoa_maxcut)
- [MaxCut tutorial in Qiskit](https://qiskit.org/documentation/tutorials/optimization/6_examples_max_cut_and_tsp.html)
- [MaxCut tutorial in PyQuil](https://grove-docs.readthedocs.io/en/latest/qaoa.html)
- [MaxCut tutorial in Cirq](https://quantumai.google/cirq/experiments/qaoa/qaoa_maxcut)