Jonathan Zoller ([email protected])

Example to demonstrate using the control library to determine control pulses using the ctrlpulseoptim.optimize_pulse_unitary function. The CRAB algorithm is used to optimize pulse shapes to minimize the fidelity error, which is equivalent maximising the fidelity to an optimal value of 1.

The system in this example are two qubits, where the interaction can be controlled. The target is to perform a pure state transfer from a down-down state to an up-up state.

The user can experiment with the timeslicing, by means of changing the number of timeslots and/or total time for the evolution. Different initial (starting) pulse types can be tried as well as boundaries on the control and a smooth ramping of the pulse when switching the control on and off (at the beginning and close to the end). The initial and final pulses are displayed in a plot

An in depth discussion of using methods of this type can be found in [1,2]

In [1]:

```
%matplotlib inline
import numpy as np
import matplotlib.pyplot as plt
import datetime
```

In [2]:

```
from qutip import Qobj, identity, sigmax, sigmaz, tensor
import random
import qutip.logging_utils as logging
logger = logging.get_logger()
#Set this to None or logging.WARN for 'quiet' execution
log_level = logging.INFO
#QuTiP control modules
import qutip.control.pulseoptim as cpo
example_name = '2qubitInteract'
```

The dynamics of the system are governed by the combined Hamiltonian:
H(t) = H_d + sum(u1(t)*Hc1 + u2(t)*Hc2 + ....)
That is the time-dependent Hamiltonian has a constant part (called here the drift) and time vary parts, which are the control Hamiltonians scaled by some functions u_j(t) known as control amplitudes
In this example we describe an Ising like Hamiltonian, encompassing random coefficients in the drift part and controlling the interaction of the qubits:

$ \hat{H} = \sum_{i=1}^2 \alpha_i \sigma_x^i + \beta_i \sigma_z^i + u(t) \cdot \sigma_z \otimes \sigma_z $

Initial $\newcommand{\ket}[1]{\left|{#1}\right\rangle} \ket{\psi_0} = \text{U_0}$ and target state $\ket{\psi_t} = \text{U_targ}$ are chosen to be:

$ \ket{\psi_0} = \begin{pmatrix} 1 \\ 0 \\ 0 \\ 0 \end{pmatrix}$

$ \ket{\psi_t} = \begin{pmatrix} 0 \\ 0 \\ 0 \\ 1 \end{pmatrix}$

In [3]:

```
random.seed(20)
alpha = [random.random(),random.random()]
beta = [random.random(),random.random()]
Sx = sigmax()
Sz = sigmaz()
H_d = (alpha[0]*tensor(Sx,identity(2)) +
alpha[1]*tensor(identity(2),Sx) +
beta[0]*tensor(Sz,identity(2)) +
beta[1]*tensor(identity(2),Sz))
H_c = [tensor(Sz,Sz)]
# Number of ctrls
n_ctrls = len(H_c)
q1_0 = q2_0 = Qobj([[1], [0]])
q1_targ = q2_targ = Qobj([[0], [1]])
psi_0 = tensor(q1_0, q2_0)
psi_targ = tensor(q1_targ, q2_targ)
```

*H(t_k)*dt). Combining these for all the timeslots gives the approximation to the evolution from an initial state $\psi_0$ at t=0 to U(T) at the t=evo_time.
The number of timeslots and evo_time have to be chosen such that the timeslot durations (dt) are small compared with the dynamics of the system.

In [4]:

```
# Number of time slots
n_ts = 100
# Time allowed for the evolution
evo_time = 18
```

At each iteration the fidelity of the evolution is tested by comparaing the calculated evolution U(T) with the target U_targ. For unitary systems such as this one this is typically: f = normalise(overlap(U(T), U_targ)). The maximum fidelity (for a unitary system) calculated this way would be 1, and hence the error is calculated as fid_err = 1 - fidelity. As such the optimisation is considered completed when the fid_err falls below such a target value.

In some cases the optimisation either gets stuck in some local minima, or the fid_err_targ is just not achievable, therefore some limits are set to the time/effort allowed to find a solution.

The algorithm uses the CRAB algorithm to determine optimized coefficients that lead to a minimal fidelity error. The underlying optimization procedure is set to be the Nelder-Mead downhill simplex. Therefore, when all vertices shrink together, the algorithm will terminate.

In [5]:

```
# Fidelity error target
fid_err_targ = 1e-3
# Maximum iterations for the optisation algorithm
max_iter = 500
# Maximum (elapsed) time allowed in seconds
max_wall_time = 120
```

In [6]:

```
# pulse type alternatives: RND|ZERO|LIN|SINE|SQUARE|SAW|TRIANGLE|
p_type = 'DEF'
```

In [7]:

```
#Set to None to suppress output files
f_ext = "{}_n_ts{}_ptype{}.txt".format(example_name, n_ts, p_type)
```

In [8]:

```
result = cpo.opt_pulse_crab_unitary(H_d, H_c, psi_0, psi_targ, n_ts, evo_time,
fid_err_targ=fid_err_targ,
max_iter=max_iter, max_wall_time=max_wall_time,
init_coeff_scaling=5.0, num_coeffs=5,
method_params={'xtol':1e-3},
guess_pulse_type=None, guess_pulse_action='modulate',
out_file_ext=f_ext,
log_level=log_level, gen_stats=True)
```

Firstly the performace statistics are reported, which gives a breakdown of the processing times. In this example it can be seen that the majority of time is spent calculating the propagators, i.e. exponentiating the combined Hamiltonian.

The optimised U(T) is reported as the 'final evolution', which is essentially the string representation of the Qobj that holds the full time evolution at the point when the optimisation is terminated.

The key information is in the summary (given last). Here the final fidelity is reported and the reason for termination of the algorithm.

In [9]:

```
result.stats.report()
print("Final evolution\n{}\n".format(result.evo_full_final))
print("********* Summary *****************")
print("Final fidelity error {}".format(result.fid_err))
print("Final gradient normal {}".format(result.grad_norm_final))
print("Terminated due to {}".format(result.termination_reason))
print("Number of iterations {}".format(result.num_iter))
print("Completed in {} HH:MM:SS.US".format(
datetime.timedelta(seconds=result.wall_time)))
```

In [11]:

```
fig1 = plt.figure()
ax1 = fig1.add_subplot(2, 1, 1)
ax1.set_title("Initial Control amps")
ax1.set_ylabel("Control amplitude")
ax1.step(result.time,
np.hstack((result.initial_amps[:, 0], result.initial_amps[-1, 0])),
where='post')
ax2 = fig1.add_subplot(2, 1, 2)
ax2.set_title("Optimised Control Amplitudes")
ax2.set_xlabel("Time")
ax2.set_ylabel("Control amplitude")
ax2.step(result.time,
np.hstack((result.final_amps[:, 0], result.final_amps[-1, 0])),
where='post')
plt.show()
```

In [12]:

```
from qutip.ipynbtools import version_table
version_table()
```

Out[12]:

[1] Doria, P., Calarco, T. & Montangero, S.: Optimal Control Technique for Many-Body Quantum Dynamics. Phys. Rev. Lett. 106, 1–4 (2011).

[2] Caneva, T., Calarco, T. & Montangero, S.: Chopped random-basis quantum optimization. Phys. Rev. A - At. Mol. Opt. Phys. 84, (2011).

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