#!/usr/bin/env python
# coding: utf-8

# # Time-dependent Master Equation: Landau-Zener transitions

# J.R. Johansson and P.D. Nation
# 
# For more information about QuTiP see [http://qutip.org](http://qutip.org)

# In[1]:


import time

import matplotlib.pyplot as plt
import numpy as np
from qutip import (Odeoptions, about, basis, destroy, expect, mesolve,
                   propagator, propagator_steadystate, sigmax, sigmaz)

get_ipython().run_line_magic('matplotlib', 'inline')


# In[2]:


def hamiltonian_t(t, args):
    """evaluate the hamiltonian at time t."""
    H0 = args[0]
    H1 = args[1]

    return H0 + t * H1


# In[3]:


def qubit_integrate(delta, eps0, A, gamma1, gamma2, psi0, tlist):

    # Hamiltonian
    sx = sigmax()
    sz = sigmaz()
    sm = destroy(2)

    H0 = -delta / 2.0 * sx - eps0 / 2.0 * sz
    H1 = -A / 2.0 * sz

    # collapse operators
    c_op_list = []

    n_th = 0.0  # zero temperature

    # relaxation
    rate = gamma1 * (1 + n_th)
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm)

    # excitation
    rate = gamma1 * n_th
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm.dag())

    # dephasing
    rate = gamma2
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sz)

    # evolve and calculate expectation values

    # method 1: function callback which returns the time-depdent qobj
    # H_args = (H0, H1)
    # output = mesolve(hamiltonian_t,
    #                  psi0, tlist, c_op_list, [sm.dag() * sm], H_args)

    # method 2: a function callback that returns the coefficient for a qobj
    # H = [H0, [H1, lambda x,y: x]]
    # output = mesolve(H, psi0, tlist, c_op_list, [sm.dag() * sm], {})

    # method 3: a string that defines the coefficient. The solver generates
    # and compiles C code using cython. This method is usually the fastest
    # for large systems or long time evolutions, but there is fixed-time
    # overhead that makes it inefficient for small and short-time evolutions.
    H = [H0, [H1, "t"]]
    output = mesolve(H, psi0, tlist, c_op_list, [sm.dag() * sm], {})

    return output.expect[0]


# In[4]:


#
# set up the calculation
#
delta = 0.5 * 2 * np.pi  # qubit sigma_x coefficient
eps0 = 0.0 * 2 * np.pi  # qubit sigma_z coefficient
A = 2.0 * 2 * np.pi  # sweep rate
gamma1 = 0.0  # relaxation rate
gamma2 = 0.0  # dephasing  rate
psi0 = basis(2, 0)  # initial state

tlist = np.linspace(-20.0, 20.0, 5000)


# In[5]:


start_time = time.time()
p_ex = qubit_integrate(delta, eps0, A, gamma1, gamma2, psi0, tlist)
print("time elapsed = " + str(time.time() - start_time))


# In[6]:


fig, ax = plt.subplots(figsize=(12, 8))
ax.plot(tlist, np.real(p_ex), "b", tlist, np.real(1 - p_ex), "r")
ax.plot(tlist, 1 - np.exp(-np.pi * delta**2 / (2 * A)) *
        np.ones(tlist.shape[0]), "k")
ax.set_xlabel("Time")
ax.set_ylabel("Occupation probability")
ax.set_title("Landau-Zener transition")
ax.legend(("Excited state", "Ground state", "Landau-Zener formula"), loc=0);


# ## Steady state of strongly driven two-level system (repeated LZ transitions)

# In[7]:


def qubit_integrate(delta, eps0, A, omega, gamma1,
                    gamma2, psi0, tlist, option):

    # Hamiltonian
    sx = sigmax()
    sz = sigmaz()
    sm = destroy(2)

    H0 = -delta / 2.0 * sx - eps0 / 2.0 * sz
    H1 = -A / 2.0 * sz

    H = [H0, [H1, "cos(w*t)"]]
    H_args = {"w": omega}
    # collapse operators
    c_op_list = []

    n_th = 0.0  # zero temperature

    # relaxation
    rate = gamma1 * (1 + n_th)
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm)

    # excitation
    rate = gamma1 * n_th
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm.dag())

    # dephasing
    rate = gamma2
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sz)

    if option == "dynamics":
        # evolve and calculate expectation values
        output = mesolve(H, psi0, tlist, c_op_list, [sm.dag() * sm], H_args)

        return output.expect[0]

    else:  # option = steadystate

        # find the propagator for one driving period
        T = 2 * np.pi / omega
        U = propagator(H, T, c_op_list, H_args,
                       options=Odeoptions(nsteps=2500))

        # find the steady state of successive application of the propagator
        rho_ss = propagator_steadystate(U)

        return np.real(expect(sm.dag() * sm, rho_ss))


# In[8]:


#
# set up the calculation: a strongly driven two-level system
# (repeated LZ transitions)
#
delta = 0.05 * 2 * np.pi  # qubit sigma_x coefficient
eps0 = 0.0 * 2 * np.pi  # qubit sigma_z coefficient
A = 2.0 * 2 * np.pi  # sweep rate
gamma1 = 0.0001  # relaxation rate
gamma2 = 0.005  # dephasing  rate
psi0 = basis(2, 0)  # initial state
omega = 0.05 * 2 * np.pi  # driving frequency
T = (2 * np.pi) / omega  # driving period

tlist = np.linspace(0.0, 3 * T, 1500)


# ### Steady state and dynamics for a fixed driving amplitude

# In[9]:


start_time = time.time()
p_ex = qubit_integrate(delta, eps0, A, omega, gamma1,
                       gamma2, psi0, tlist, "dynamics")
print("dynamics: time elapsed = " + str(time.time() - start_time))


# In[10]:


start_time = time.time()
p_ex_ss = qubit_integrate(
    delta, eps0, A, omega, gamma1, gamma2, psi0, tlist, "steadystate"
)
print("steady state: time elapsed = " + str(time.time() - start_time))


# In[11]:


fig, (ax1, ax2) = plt.subplots(2, 1, figsize=(12, 8))

ax1.plot(
    tlist,
    np.real(p_ex),
    "b",
    tlist,
    np.real(1 - p_ex),
    "r",
    tlist,
    np.ones(np.shape(tlist)) * p_ex_ss,
    "k",
)
ax1.set_xlabel("Time")
ax1.set_ylabel("Probability")
ax1.set_title("Repeated Landau-Zener-like transitions")
ax1.legend(("Excited state", "Ground state", "Excited steady state"), loc=0)

ax2.plot(tlist, -delta / 2.0 * np.ones(np.shape(tlist)), "r")
ax2.plot(tlist, -(eps0 / 2.0 + A / 2.0 * np.cos(omega * tlist)), "b")
ax2.legend(("sx coeff", "sz coeff"))
ax2.set_xlabel("Time")
ax2.set_ylabel("Coefficients in the Hamiltonian");


# ### Steady state as a function of driving amplitude

# In[12]:


start_time = time.time()

# increase the number of points and the range
# to obtain a more detailed result
# note that this increases the calculation time
A_vec = 2 * np.pi * np.linspace(1.9, 2.1, 5)

p_ex_ss_vec = np.zeros(len(A_vec))
idx = 0
start_time = time.time()
for A in A_vec:
    print(A)

    p_ex_ss_vec[idx] = qubit_integrate(
        delta, eps0, A, omega, gamma1, gamma2, psi0, tlist, "steadystate"
    )
    idx += 1

print("time elapsed = " + str(time.time() - start_time))


# In[13]:


fig, ax = plt.subplots()

ax.plot(A_vec / (2 * np.pi), p_ex_ss_vec, "b.-")
ax.set_title("Steady state of repeated LZ transitions")
ax.set_xlabel("driving amplitude")
ax.set_ylabel("Occupation probability");


# ## Steadystate of a strongly driven two-level system as a function of driving amplitude and qubit bias

# Find the steady state of a strongly driven qubit as a function of driving amplitude and qubit bias. 
# 
# Note: This calculation can takes a long time.

# In[14]:


def sd_qubit_integrate(delta, eps0_vec, A_vec, w, gamma1, gamma2):

    # Hamiltonian
    sx = sigmax()
    sz = sigmaz()
    sm = destroy(2)

    # collapse operators
    c_op_list = []

    n_th = 0.0  # zero temperature

    # relaxation
    rate = gamma1 * (1 + n_th)
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm)

    # excitation
    rate = gamma1 * n_th
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sm.dag())

    # dephasing
    rate = gamma2
    if rate > 0.0:
        c_op_list.append(np.sqrt(rate) * sz)

    N = len(A_vec)
    M = len(eps0_vec)
    p_ex = np.zeros([N, M])  # , dtype=complex)

    T = 2 * np.pi / w

    sn = sm.dag() * sm

    # sweep over the driving amplitude and bias point, find the steady state
    # for each point and store in a matrix
    for n in range(0, N):
        for m in range(0, M):

            H0 = -delta / 2.0 * sx - eps0_vec[m] / 2.0 * sz
            H1 = -A_vec[n] * sx

            H = [H0, [H1, "sin(w * t)"]]

            H_args = {"w": omega}

            # find the propagator for one period of the time-dependent
            # hamiltonian
            U = propagator(H, T, c_op_list, H_args)

            # find the steady state of the driven system
            rho_ss = propagator_steadystate(U)

            p_ex[n, m] = np.real(expect(sn, rho_ss))

    return p_ex


# In[15]:


#
# set up the parameters
#
delta = 0.2 * 2 * np.pi  # qubit sigma_x coefficient
w = 1.0 * 2 * np.pi  # qubit sigma_z coefficient

A_vec = np.linspace(0.0, 4.0, 3) * 2 * np.pi  # driving amplitude
eps0_vec = np.linspace(0.0, 4.0, 3) * 2 * np.pi  # qubit sigma-z bias point

gamma1 = 0.05  # relaxation rate
gamma2 = 0.0  # dephasing  rate


# In[16]:


start_time = time.time()
p_ex = sd_qubit_integrate(delta, eps0_vec, A_vec, w, gamma1, gamma2)
print("time elapsed = " + str(time.time() - start_time))


# In[17]:


fig, ax = plt.subplots(figsize=(10, 10))
p = ax.pcolor(A_vec, eps0_vec, np.real(p_ex), shading="auto")
p.set_cmap("RdYlBu_r")
ax.set_ylabel(r"$A/\omega$", fontsize=20)
ax.set_xlabel(r"$\epsilon_0/\omega$", fontsize=20)
ax.axis("tight")
ax.set_title("Excitation probabilty of qubit, in steady state", fontsize=16);


# ## Versions

# In[18]:


about()


# In[ ]: