master-thesis/python/richard_hops/energy_flow.org
2021-10-20 16:13:32 +02:00

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Setup

Jupyter

  %load_ext autoreload
  %autoreload 2
  %load_ext jupyter_spaces
The autoreload extension is already loaded. To reload it, use:
  %reload_ext autoreload
The jupyter_spaces extension is already loaded. To reload it, use:
  %reload_ext jupyter_spaces

Matplotlib

  import matplotlib
  import matplotlib.pyplot as plt

  #matplotlib.use("TkCairo", force=True)
  %gui tk
  %matplotlib inline
  plt.style.use('ggplot')

Richard (old) HOPS

  import hierarchyLib
  import hierarchyData
  import numpy as np

  from stocproc.stocproc import StocProc_FFT
  import bcf
  from dataclasses import dataclass
  import scipy
  import scipy.misc
  import scipy.signal

Auxiliary Definitions

  σ1 = np.matrix([[0,1],[1,0]])
  σ2 = np.matrix([[0,-1j],[1j,0]])
  σ3 = np.matrix([[1,0],[0,-1]])

Model Setup

Basic parameters.

  γ = 5 # coupling ratio
  ω_c = 1  # center of spect. dens
  δ = 1  # breadth BCF
  t_max = 10
  t_steps = 500
  k_max = 2
  seed = 100
  H_s = σ3 + np.eye(2)
  L =  1 / 2 * (σ1 - 1j * σ2) * γ
  ψ_0 = np.array([1, 0])
  W = ω_c * 1j + δ  # exponent BCF
  N = 100

BCF

  @dataclass
  class CauchyBCF:
      δ: float
      ω_c: float

      def I(self, ω):
          return np.sqrt(self.δ) / (self.δ + (ω - self.ω_c) ** 2 / self.δ)

      def __call__(self, τ):
          return np.sqrt(self.δ) * np.exp(-1j * self.ω_c * τ - np.abs(τ) * self.δ)

      def __bfkey__(self):
          return self.δ, self.ω_c

  α = CauchyBCF(δ, ω_c)

Plot

  %%space plot
  t = np.linspace(0, t_max, 1000)
  ω = np.linspace(ω_c - 10, ω_c + 10, 1000)
  fig, axs = plt.subplots(2)
  axs[0].plot(t, np.real(α(t)))
  axs[0].plot(t, np.imag(α(t)))
  axs[1].plot(ω, α.I(ω))
<matplotlib.lines.Line2D at 0x7f6be57ecfd0>
<matplotlib.lines.Line2D at 0x7f6be579f8e0>
<matplotlib.lines.Line2D at 0x7f6bf5de3430>

/hiro/master-thesis/media/commit/e714b65ad3a2b056d7d0bef1cc450ce7dc177eee/python/richard_hops/.ob-jupyter/252b4713c37e957d1909f4354fd107d3803ecda2.png

Hops setup

  HierachyParam = hierarchyData.HiP(
      k_max=k_max,
      # g_scale=None,
      # sample_method='random',
      seed=seed,
      nonlinear=False,
      # normalized=False,
      # terminator=False,
      result_type=hierarchyData.RESULT_TYPE_ALL,
      # accum_only=None,
      # rand_skip=None
  )

Integration.

  IntegrationParam = hierarchyData.IntP(
      t_max=t_max,
      t_steps=t_steps,
      # integrator_name='zvode',
      # atol=1e-8,
      # rtol=1e-8,
      # order=5,
      # nsteps=5000,
      # method='bdf',
      # t_steps_skip=1
  )

And now the system.

  SystemParam = hierarchyData.SysP(
      H_sys=H_s,
      L=L,
      psi0=ψ_0,  # excited qubit
      g=np.array([np.sqrt(δ)]),
      w=np.array([W]),
      H_dynamic=[],
      bcf_scale=1,  # some coupling strength (scaling of the fit parameters 'g_i')
      gw_hash=None,  # this is used to load g,w from some database
      len_gw=1,
  )

The quantum noise.

  Eta = StocProc_FFT(
      α.I,
      t_max,
      α,
      negative_frequencies=True,
      seed=seed,
      intgr_tol=1e-2,
      intpl_tol=1e-2,
      scale=1,
  )
  stocproc.stocproc - INFO - use neg freq
  stocproc.method_ft - INFO - get_dt_for_accurate_interpolation, please wait ...
  stocproc.method_ft - INFO - acc interp N 33 dt 2.88e-01 -> diff 7.57e-03
  stocproc.method_ft - INFO - requires dt < 2.878e-01
  stocproc.method_ft - INFO - get_N_a_b_for_accurate_fourier_integral, please wait ...
  stocproc.method_ft - INFO - J_w_min:1.00e-02 N 32 yields: interval [-8.95e+00,1.09e+01] diff 2.01e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 32 yields: interval [-3.06e+01,3.26e+01] diff 6.40e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-02 N 64 yields: interval [-8.95e+00,1.09e+01] diff 2.00e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 32 yields: interval [-9.90e+01,1.01e+02] diff 1.90e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 64 yields: interval [-3.06e+01,3.26e+01] diff 1.31e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-02 N 128 yields: interval [-8.95e+00,1.09e+01] diff 2.00e-01
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 32 yields: interval [-3.15e+02,3.17e+02] diff 2.68e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 64 yields: interval [-9.90e+01,1.01e+02] diff 1.15e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 128 yields: interval [-3.06e+01,3.26e+01] diff 6.33e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-02 N 256 yields: interval [-8.95e+00,1.09e+01] diff 2.00e-01
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 32 yields: interval [-9.99e+02,1.00e+03] diff 2.99e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 64 yields: interval [-3.15e+02,3.17e+02] diff 2.29e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 128 yields: interval [-9.90e+01,1.01e+02] diff 4.21e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 256 yields: interval [-3.06e+01,3.26e+01] diff 6.33e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-02 N 512 yields: interval [-8.95e+00,1.09e+01] diff 2.00e-01
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-07 N 32 yields: interval [-3.16e+03,3.16e+03] diff 3.09e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 64 yields: interval [-9.99e+02,1.00e+03] diff 2.84e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 128 yields: interval [-3.15e+02,3.17e+02] diff 1.66e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 256 yields: interval [-9.90e+01,1.01e+02] diff 5.63e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 512 yields: interval [-3.06e+01,3.26e+01] diff 6.33e-02
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-08 N 32 yields: interval [-1.00e+04,1.00e+04] diff 3.13e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-07 N 64 yields: interval [-3.16e+03,3.16e+03] diff 3.04e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 128 yields: interval [-9.99e+02,1.00e+03] diff 2.57e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 256 yields: interval [-3.15e+02,3.17e+02] diff 8.81e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 512 yields: interval [-9.90e+01,1.01e+02] diff 2.00e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 1024 yields: interval [-3.06e+01,3.26e+01] diff 6.33e-02
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-09 N 32 yields: interval [-3.16e+04,3.16e+04] diff 3.14e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-08 N 64 yields: interval [-1.00e+04,1.00e+04] diff 3.11e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-07 N 128 yields: interval [-3.16e+03,3.16e+03] diff 2.95e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 256 yields: interval [-9.99e+02,1.00e+03] diff 2.10e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 512 yields: interval [-3.15e+02,3.17e+02] diff 2.47e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 1024 yields: interval [-9.90e+01,1.01e+02] diff 2.00e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-03 N 2048 yields: interval [-3.06e+01,3.26e+01] diff 6.33e-02
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-10 N 32 yields: interval [-1.00e+05,1.00e+05] diff 3.14e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-09 N 64 yields: interval [-3.16e+04,3.16e+04] diff 3.13e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-08 N 128 yields: interval [-1.00e+04,1.00e+04] diff 3.08e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-07 N 256 yields: interval [-3.16e+03,3.16e+03] diff 2.77e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 512 yields: interval [-9.99e+02,1.00e+03] diff 1.41e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 1024 yields: interval [-3.15e+02,3.17e+02] diff 1.94e-02
  stocproc.method_ft - INFO - J_w_min:1.00e-04 N 2048 yields: interval [-9.90e+01,1.01e+02] diff 2.00e-02
  stocproc.method_ft - INFO - increasing N while shrinking the interval does lower the error -> try next level
  stocproc.method_ft - INFO - J_w_min:1.00e-11 N 32 yields: interval [-3.16e+05,3.16e+05] diff 3.14e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-10 N 64 yields: interval [-1.00e+05,1.00e+05] diff 3.14e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-09 N 128 yields: interval [-3.16e+04,3.16e+04] diff 3.12e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-08 N 256 yields: interval [-1.00e+04,1.00e+04] diff 3.02e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-07 N 512 yields: interval [-3.16e+03,3.16e+03] diff 2.44e+00
  stocproc.method_ft - INFO - J_w_min:1.00e-06 N 1024 yields: interval [-9.99e+02,1.00e+03] diff 6.29e-01
  stocproc.method_ft - INFO - J_w_min:1.00e-05 N 2048 yields: interval [-3.15e+02,3.17e+02] diff 6.32e-03
  stocproc.method_ft - INFO - return, cause tol of 0.01 was reached
  stocproc.method_ft - INFO - requires dx < 3.088e-01
  stocproc.stocproc - INFO - Fourier Integral Boundaries: [-3.152e+02, 3.172e+02]
  stocproc.stocproc - INFO - Number of Nodes            : 2048
  stocproc.stocproc - INFO - yields dx                  : 3.088e-01
  stocproc.stocproc - INFO - yields dt                  : 9.935e-03
  stocproc.stocproc - INFO - yields t_max               : 2.034e+01

Actual Hops

Generate the key for binary caching.

  hi_key = hierarchyData.HIMetaKey_type(
      HiP=HierachyParam,
      IntP=IntegrationParam,
      SysP=SystemParam,
      Eta=Eta,
      EtaTherm=None,
  )

Initialize Hierarchy.

  myHierarchy = hierarchyLib.HI(hi_key, number_of_samples=N, desc="run a test case")
init Hi class, use 6 equation
/home/hiro/Documents/Projects/UNI/master/masterarb/python/richard_hops/hierarchyLib.py:1058: UserWarning: sum_k_max is not implemented! DO SO BEFORE NEXT USAGE (use simplex).HierarchyParametersType does not yet know about sum_k_max
  warnings.warn(

Run the integration.

  myHierarchy.integrate_simple(data_name="energy_flow.data")
samples     :0.0%
integration :0.0%
samples     : 100%
integration :0.0%


Get the samples.

  # to access the data the 'hi_key' is used to find the data in the hdf5 file
  with hierarchyData.HIMetaData(hid_name="energy_flow.data", hid_path=".") as metaData:
      with metaData.get_HIData(hi_key, read_only=True) as data:
          smp = data.get_samples()
          print("{} samples found in database".format(smp))
          τ = data.get_time()
          rho_τ = data.get_rho_t()
          s_proc = np.array(data.stoc_proc)
          states = np.array(data.aux_states).copy()
          ψ_1 = np.array(data.aux_states)[:, :, 0:2]
          ψ_0 = np.array(data.stoc_traj)
          y = np.array(data.y)
122 samples found in database

Calculate energy.

  energy = np.array([np.trace(ρ * H_s).real/np.trace(ρ).real for ρ in rho_τ])
  plt.plot(τ, energy)
<matplotlib.lines.Line2D at 0x7f6bf5cdef10>

/hiro/master-thesis/media/commit/e714b65ad3a2b056d7d0bef1cc450ce7dc177eee/python/richard_hops/.ob-jupyter/009521d0047fb3d6927063413a3290f039a1cbe3.png

  %%space plot
  plt.plot(τ, np.trace(rho_τ.T).real)
<matplotlib.lines.Line2D at 0x7f6bf5be1700>

/hiro/master-thesis/media/commit/e714b65ad3a2b056d7d0bef1cc450ce7dc177eee/python/richard_hops/.ob-jupyter/6b4898a15426ff4e99c43e8db1649e9fe9f1ec28.png

Energy Flow

  ψ_1.shape
160 500 2

Let's look at the norm.

  plt.plot(τ, (ψ_1[0].conj() * ψ_1[0]).sum(axis=1).real)
<matplotlib.lines.Line2D at 0x7f6bf5a5d280>

/hiro/master-thesis/media/commit/e714b65ad3a2b056d7d0bef1cc450ce7dc177eee/python/richard_hops/.ob-jupyter/542a9e20ddb61f23548be094780da540cd1d60b2.png

And try to calculate the energy flow.

  def flow_for_traj(ψ_0, ψ_1):
      a = np.array((L @ ψ_0.T).T)

      return np.array(2 * (1j * -W * np.sum(a.conj() * ψ_1, axis=1)).real).flatten()


  def flow_for_traj_alt(ψ_0, y):
      Eta.new_process(y)
      eta_dot = scipy.misc.derivative(Eta, τ, dx=1e-6)
      a = L @ ψ_0.T

      return (
          eta_dot * np.array(2 * (1j * np.sum(ψ_0.conj() * a, axis=1))).flatten()
      ).real

Now we calculate the average over all trajectories.

  j = np.zeros_like(τ)
  for i in range(0, N):
      j += flow_for_traj(ψ_0[i], ψ_1[i])
  j /= N

And do the same with the alternative implementation.

  ja = np.zeros_like(τ)
  for i in range(0, N):
      ja += flow_for_traj_alt(ψ_0[i], y[i])
  ja /= N

And plot it :)

  %matplotlib inline
  plt.plot(τ, j)
  #plt.plot(τ, ja)
  plt.show()

/hiro/master-thesis/media/commit/e714b65ad3a2b056d7d0bef1cc450ce7dc177eee/python/richard_hops/.ob-jupyter/750be1a5e9455c104056c0615334e80853388e20.png

Let's calculate the integrated energy.

  E_t = np.array([0] + [scipy.integrate.simpson(j[0:n], τ[0:n]) for n in range(1, len(τ))])
  E_t[-1]
1.999601704648048

With this we can retrieve the energy of the interaction Hamiltonian.

  E_I = 2 - energy - E_t
  %%space plot
  plt.rcParams['figure.figsize'] = [15, 10]
  #plt.plot(τ, j, label="$J$", linestyle='--')
  plt.plot(τ, E_t, label=r"$\langle H_{\mathrm{B}}\rangle$")
  plt.plot(τ, E_I, label=r"$\langle H_{\mathrm{I}}\rangle$")
  plt.plot(τ, energy, label=r"$\langle H_{\mathrm{S}}\rangle$")

  plt.xlabel("τ")
  plt.legend()
  plt.show()
<matplotlib.lines.Line2D at 0x7f6bcb4ce610>
<matplotlib.lines.Line2D at 0x7f6bcb4cea60>
<matplotlib.lines.Line2D at 0x7f6bcb4ce7f0>
Text(0.5, 0, 'τ')
<matplotlib.legend.Legend at 0x7f6bcb4da160>

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#+RESULTS: