mirror of
https://github.com/vale981/HOPSFlow-Paper
synced 2025-03-04 17:21:42 -05:00
horrible: tabula raza
This commit is contained in:
parent
aa3ae06cd8
commit
b1bfb91e81
129 changed files with 290091 additions and 186436 deletions
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@ -18,7 +18,14 @@ val_path = Path(os.getcwd()) / "values"
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def export_fig(
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name, fig=None, x_scaling=1, y_scaling=0.4, tikz=True, save_pickle=True, **kwargs
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name,
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fig=None,
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x_scaling=1,
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y_scaling=0.4,
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tikz=True,
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save_pickle=True,
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data=None,
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**kwargs,
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):
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fig_path.mkdir(parents=True, exist_ok=True)
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if fig is None:
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@ -51,6 +58,10 @@ def export_fig(
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with open(fig_path / f"{name}.pickle", "wb") as file:
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pickle.dump(fig, file)
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if data is not None:
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with open(fig_path / f"{name}.data.pickle", "wb") as file:
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pickle.dump(data, file)
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def scientific_round(val, *err, retprec=False):
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"""Scientifically rounds the values to the given errors."""
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@ -145,16 +156,16 @@ MPL_RC = {
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"axes.labelcolor": "black",
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"xtick.color": "black",
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"ytick.color": "black",
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"figure.figsize": (3.4, 3.2),
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"figure.figsize": (5.78, 2.4),
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"text.usetex": True,
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"font.family": "serif",
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# "font.serif": ["Roman"],
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"font.size": 9,
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"axes.labelsize": 10,
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"axes.titlesize": 10,
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"legend.fontsize": 9,
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"xtick.labelsize": 8,
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"ytick.labelsize": 8,
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"font.size": 15,
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"axes.labelsize": 13,
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"axes.titlesize": 15,
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"legend.fontsize": 13,
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"xtick.labelsize": 13,
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"ytick.labelsize": 13,
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"figure.constrained_layout.use": True,
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# "text.latex.preamble": r"\usepackage{mathtools}",
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}
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@ -17,7 +17,9 @@ def plot_power_eff_convergence(models, steady_idx=2):
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try:
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Ns = model.power(steady_idx=steady_idx).Ns
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a_power.plot(Ns, model.power(steady_idx=steady_idx).values)
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a_efficiency.plot(Ns, np.abs(model.efficiency(steady_idx=steady_idx).values))
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a_efficiency.plot(
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Ns, np.abs(model.efficiency(steady_idx=steady_idx).values)
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)
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except:
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pass
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@ -449,6 +451,58 @@ def plot_3d_heatmap(models, value_accessor, x_spec, y_spec, normalize=False, ax=
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ax.set_yticks(y_labels)
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@pu.wrap_plot
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def plot_contour(
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models, value_accessor, x_spec, y_spec, normalize=False, ax=None, levels=None
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):
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value_dict = {}
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x_labels = set()
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y_labels = set()
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for model in models:
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x_label = x_spec(model)
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y_label = y_spec(model)
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value = value_accessor(model)
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if x_label not in value_dict:
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value_dict[x_label] = {}
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if y_label in value_dict[x_label]:
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raise ValueError(
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f"Dublicate value for model with x={x_label}, y={y_label}."
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)
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value_dict[x_label][y_label] = value_accessor(model)
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x_labels.add(x_label)
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y_labels.add(y_label)
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x_labels = np.sort(list(x_labels))
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y_labels = np.sort(list(y_labels))
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_xx, _yy = np.meshgrid(x_labels, y_labels, indexing="ij")
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x, y = _xx.ravel(), _yy.ravel()
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values = (
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np.fromiter((value_dict[_x][_y] for _x, _y in zip(x, y)), dtype=float)
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.reshape(len(x_labels), len(y_labels))
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.T
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)
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normalized_values = abs(values) - abs(values).min()
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normalized_values /= abs(normalized_values).max()
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cont = ax.contourf(
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x_labels,
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y_labels,
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values / abs(values).max() if normalize else values,
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levels=levels,
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)
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ax.set_xticks(x_labels)
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ax.set_yticks(y_labels)
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return cont, (x_labels, y_labels, values)
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def val_relative_to_steady(model, val, steady_idx, shift=0):
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shift_idx = int(1 / model.dt * shift)
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begin_idx = model.strobe[1][steady_idx] - shift_idx
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@ -578,3 +632,20 @@ def plot_bloch_components(model, ax=None, **kwargs):
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)
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ax.legend()
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ax.set_xlabel(r"$\tau$")
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@pu.wrap_plot
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def plot_energy_deviation(models, ax=None, labels=None):
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ax.set_xlabel(r"$\tau$")
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ax.set_ylabel(r"$\Delta||H||/\max||H||$")
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for i, model in enumerate(models):
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ax.plot(
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model.t,
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abs(model.total_energy_from_power().value - model.total_energy().value)
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/ max(abs(model.total_energy_from_power().value)),
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label=labels[i] if labels else None,
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)
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if labels:
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ax.legend()
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python/otto_motor/subprojects/bath_memory/.data.b/model_data.json
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@ -41,12 +41,12 @@ z
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After Width: | Height: | Size: 250 KiB |
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Before Width: | Height: | Size: 253 KiB |
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@ -115,24 +115,11 @@ coupling-change/cycle time.
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fig, ax = plt.subplots()
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for model in models:
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pu.plot_with_σ(models[0].t, model.interaction_power().sum_baths().integrate(model.t), ax=ax)
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print(model.system_energy().N, model.power(steady_idx=2).value, model.T[0], model.ω_c[0])
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#print(model.system_energy().N, model.power(steady_idx=2).value, model.T[0], model.ω_c[0])
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#+end_src
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#+RESULTS:
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#+begin_example
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100000 -0.0035488097495756884 0.4 0.5
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100000 -0.0030230702698324334 0.45 0.5
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90000 -0.0025068620989412353 0.5 0.5
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90000 -0.0020493778751333913 0.55 0.5
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90000 -0.001606240956288459 0.6 0.5
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90000 -0.004762254093973542 0.4 0.75
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90000 -0.004291657187886886 0.45 0.75
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90000 -0.003813983726866509 0.5 0.75
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90000 -0.0033985551697407164 0.55 0.75
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90000 -0.0029932266470821846 0.6 0.75
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90000 -0.0048136244545500416 0.4 1.0
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90000 -0.0043606909182305875 0.45 1.0
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#+end_example
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[[file:./.ob-jupyter/5a3bab0efb62516d5f68e6b330770c6fd8740bf7.svg]]
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#+begin_src jupyter-python
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@ -145,12 +132,14 @@ coupling-change/cycle time.
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[[file:./.ob-jupyter/d309a0f5287133736614819b4698027c92c12fe1.svg]]
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#+begin_src jupyter-python
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for model in models:
|
||||
plt.plot(model.t, abs(model.total_energy_from_power().value - model.total_energy().value))
|
||||
ot.plot_energy_deviation(models)
|
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#+end_src
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#+RESULTS:
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[[file:./.ob-jupyter/fa5ec90259d514bc84e5cf15ec64944bfdb1c630.svg]]
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:RESULTS:
|
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| <Figure | size | 340x320 | with | 1 | Axes> | <AxesSubplot: | xlabel= | $\tau$ | ylabel= | $\Delta | | H | | /\max | | H | | $ | > |
|
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[[file:./.ob-jupyter/c04269e0edbcb54c512e19b6da56f23825778a43.svg]]
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:END:
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#+begin_src jupyter-python
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|
|
@ -177,7 +166,7 @@ coupling-change/cycle time.
|
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#+end_src
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#+RESULTS:
|
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[[file:./.ob-jupyter/1d23b5f9499d588049ff6ab13eddc9eadcfa3c5a.svg]]
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[[file:./.ob-jupyter/a25ccbba91487a7d4ac757e0527d502a790830b1.svg]]
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#+begin_src jupyter-python
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fig, ax = plt.subplots()
|
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|
|
@ -207,7 +196,7 @@ coupling-change/cycle time.
|
|||
#+end_src
|
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|
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#+RESULTS:
|
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[[file:./.ob-jupyter/0d27f2d2ae508238056da203e2ca2ec9c08014bc.svg]]
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[[file:./.ob-jupyter/6037d87d2d4f3519db8d960319384d87040a33b8.svg]]
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#+begin_src jupyter-python
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|
|
@ -389,6 +378,58 @@ coupling-change/cycle time.
|
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[[file:./.ob-jupyter/92eb14fc6298a31f763a69186ae203923187aa38.svg]]
|
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:END:
|
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#+begin_src jupyter-python
|
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f=ot.plot_contour(
|
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models,
|
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lambda model: np.clip(-model.power(steady_idx=2).value, 0, np.inf),
|
||||
lambda model: model.T[0],
|
||||
lambda model: model.ω_c[0],
|
||||
levels=10
|
||||
)
|
||||
plt.gcf().colorbar(f[2][0])
|
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#+end_src
|
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|
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#+RESULTS:
|
||||
:RESULTS:
|
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: <matplotlib.colorbar.Colorbar at 0x7ff4ac4da4c0>
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[[file:./.ob-jupyter/ac6550b4f2034c623c6f1ba7c59ec20ae037eccd.svg]]
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:END:
|
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#+begin_src jupyter-python
|
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f = plt.figure()
|
||||
a_power = f.add_subplot(121)
|
||||
a_efficiency = f.add_subplot(122)
|
||||
axs = [a_power, a_efficiency]
|
||||
|
||||
for ax in axs:
|
||||
ax.set_xlabel(r"$T_c$")
|
||||
ax.set_ylabel(r"$\omega_c$")
|
||||
|
||||
(_, _, (c1, data1)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(-model.power(steady_idx=2).value, 0, np.inf),
|
||||
lambda model: model.T[0],
|
||||
lambda model: model.ω_c[0],
|
||||
ax=a_power,
|
||||
)
|
||||
a_power.set_title(r"$\bar{P}/\Omega$")
|
||||
|
||||
|
||||
(_, _, (c2, data2)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(np.nan_to_num(model.efficiency(steady_idx=2).value * 100), 0, np.inf),
|
||||
lambda model: model.T[0],
|
||||
lambda model: model.ω_c[0],
|
||||
ax=a_efficiency,
|
||||
)
|
||||
a_efficiency.set_title(r"$\eta\, [\%]$")
|
||||
f.colorbar(c1, ax=axs[0])
|
||||
f.colorbar(c2, ax=axs[1])
|
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fs.export_fig("bath_memory_power_efficiency_contour", x_scaling=2, y_scaling=.8, data=(data1, data2))
|
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#+end_src
|
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|
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#+RESULTS:
|
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[[file:./.ob-jupyter/5fc81f79f65d63721168aba9a472c104ac45df91.svg]]
|
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|
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|
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#+begin_src jupyter-python
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|
|
@ -425,7 +466,7 @@ coupling-change/cycle time.
|
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#+end_src
|
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|
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#+RESULTS:
|
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[[file:./.ob-jupyter/fd401b4549a06638d0d95f0020299ebd09257bf5.svg]]
|
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[[file:./.ob-jupyter/306565c079f017833496fccc16e3cf4f0b20a4aa.svg]]
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* Things to Look At
|
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- power and efficiency
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|
|
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|
@ -92,63 +92,13 @@ coupling-change/cycle time.
|
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* Analysis
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#+begin_src jupyter-python
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ot.plot_energy(models[5])
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ot.plot_energy(models[5])
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#+end_src
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#+RESULTS:
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:RESULTS:
|
||||
| <Figure | size | 340x320 | with | 1 | Axes> | <AxesSubplot: | xlabel= | $\tau$ | ylabel= | Energy | > |
|
||||
[[file:./.ob-jupyter/cf041b8ceb725ae01a8a9e1c0176c6ff745c3dc7.svg]]
|
||||
:END:
|
||||
|
||||
#+begin_src jupyter-python
|
||||
for i in range(len(Θs)):
|
||||
fig, ax = plt.subplots()
|
||||
for model in models[len(δs) * i :len(δs) * (i+1)]:
|
||||
pu.plot_with_σ(model.t, model.system_energy(), ax=ax)
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
[[file:./.ob-jupyter/f446e5aaee78e8d94583cab562c7c2125470aa63.svg]]
|
||||
[[file:./.ob-jupyter/ee49c5ceb452b52f13bf8a069300f080c261b616.svg]]
|
||||
[[file:./.ob-jupyter/0cf190cd7dc8af40d9a5f4c556d89adeb0e04077.svg]]
|
||||
:END:
|
||||
|
||||
|
||||
#+begin_src jupyter-python
|
||||
for model in models:
|
||||
plt.plot(model.t, abs(model.total_energy_from_power().value - model.total_energy().value))
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/d6b9f659fcf729fe4084269c091ef875e3892bb9.svg]]
|
||||
|
||||
|
||||
#+begin_src jupyter-python
|
||||
#[model.efficiency(steady_idx=-2).value * 100 for model in models][10]
|
||||
models[10].strobe, models[1].strobe
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
| array | ((0 65 130 195)) | array | ((0 1000 2001 3001)) |
|
||||
| array | ((0 35 70 105)) | array | ((0 1000 2001 3001)) |
|
||||
|
||||
#+begin_src jupyter-python
|
||||
models[10].system_energy().N
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
: 80000
|
||||
|
||||
#+begin_src jupyter-python
|
||||
ot.plot_power_eff_convergence(models, 2)
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
| <Figure | size | 340x320 | with | 2 | Axes> | (<AxesSubplot: xlabel= $N$ ylabel= $P$ > <AxesSubplot: xlabel= $N$ ylabel= $\eta$ >) |
|
||||
[[file:./.ob-jupyter/c7dbf7eaaf7875b816c3199d9f3524d44914a695.svg]]
|
||||
[[file:./.ob-jupyter/3da29ea23fbb86d0c258f8b077c4568444a3894e.svg]]
|
||||
:END:
|
||||
|
||||
|
||||
|
|
@ -235,7 +185,7 @@ coupling-change/cycle time.
|
|||
lambda model: model.Θ,
|
||||
ax=a_work,
|
||||
)
|
||||
a_work.set_zlabel(r"$-W$")
|
||||
a_work.set_zlabel(r"$W$")
|
||||
a_work.zaxis.labelpad = 8
|
||||
|
||||
|
||||
|
|
@ -256,14 +206,140 @@ coupling-change/cycle time.
|
|||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
[[file:./.ob-jupyter/b0aa1cfccf4cd1d8ce6ef7d54830ca8f3c178da3.svg]]
|
||||
[[file:./.ob-jupyter/e4cc58ca4c704d14df7e2b38948acb0c9e47cbab.svg]]
|
||||
[[file:./.ob-jupyter/839baa7aa85839f3073dd6eb4e11584aa4f5e972.svg]]
|
||||
[[file:./.ob-jupyter/c6fa9c1a1b2fdf210a09e58f32ceb43ddfcb3791.svg]]
|
||||
[[file:./.ob-jupyter/7cd116167e67e1ecaa314c3df0e69df8d5e607be.svg]]
|
||||
[[file:./.ob-jupyter/a4fded1708431af976271eb4a82f9e521a57a7eb.svg]]
|
||||
[[file:./.ob-jupyter/55fb3469794892bbb3e378daca3aa6d7b600b239.svg]]
|
||||
[[file:./.ob-jupyter/f8981aa4603d7ef3a58555400d2a24873608ab8c.svg]]
|
||||
[[file:./.ob-jupyter/54d2889e653fd41dab4c17e9cc71bd7c03007295.svg]]
|
||||
[[file:./.ob-jupyter/6ffe6a67ffb005d5f582305846cdce6df560a1e7.svg]]
|
||||
:END:
|
||||
#+begin_src jupyter-python
|
||||
f_mean_system_power = plt.figure()
|
||||
a_mean_system_power = f_mean_system_power.add_subplot(1, 1, 1)
|
||||
|
||||
(_, _, (c_mean_sytem_power, data_mean_system_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model:
|
||||
-ot.val_relative_to_steady(model, model.system_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_system_power,
|
||||
)
|
||||
a_mean_system_power.set_title(r"$\bar{P}_\mathrm{sys}/\Omega^2$")
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
: Text(0.5, 1.0, '$\\bar{P}_\\mathrm{sys}/\\Omega^2$')
|
||||
[[file:./.ob-jupyter/8f10f47f9025c26b3b30a075c89c5cdc751d1e00.svg]]
|
||||
:END:
|
||||
|
||||
|
||||
#+begin_src jupyter-python
|
||||
f_power = plt.figure()
|
||||
a_power = f_power.add_subplot(1, 1, 1)
|
||||
f_work = plt.figure()
|
||||
a_work = f_work.add_subplot(1, 1, 1)
|
||||
f_efficiency = plt.figure()
|
||||
a_efficiency = f_efficiency.add_subplot(1, 1, 1)
|
||||
f_mean_inter_power = plt.figure()
|
||||
a_mean_inter_power = f_mean_inter_power.add_subplot(1, 1, 1)
|
||||
f_mean_system_power = plt.figure()
|
||||
a_mean_system_power = f_mean_system_power.add_subplot(1, 1, 1)
|
||||
|
||||
axs = [a_power, a_efficiency, a_work, a_mean_inter_power, a_mean_system_power]
|
||||
figs = [f_power, f_efficiency, f_work, f_mean_inter_power, f_mean_system_power]
|
||||
for ax in axs:
|
||||
ax.set_xlabel(r"$\delta$")
|
||||
ax.set_ylabel(r"$\Theta$")
|
||||
|
||||
|
||||
(_, _, (c_efficiency, data_efficiency)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(
|
||||
np.nan_to_num(model.efficiency(steady_idx=-2).value * 100), 0, np.inf
|
||||
),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_efficiency,
|
||||
)
|
||||
a_efficiency.set_title(r"$\eta$")
|
||||
|
||||
(_, _, (c_power, data_power)) =ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(-model.power(steady_idx=-2).value, 0, np.inf),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_power,
|
||||
)
|
||||
a_power.set_title(r"$\bar{P}/\Omega^2$")
|
||||
|
||||
(_, _, (c_mean_inter_power, data_mean_inter_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(
|
||||
ot.val_relative_to_steady(model, model.interaction_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
0,
|
||||
np.inf,
|
||||
),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_inter_power,
|
||||
)
|
||||
a_mean_inter_power.set_title(r"$-\bar{P}_\mathrm{int}/\Omega^2$")
|
||||
|
||||
(_, _, (c_mean_system_power, data_mean_system_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model:
|
||||
-ot.val_relative_to_steady(model, model.system_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_system_power,
|
||||
)
|
||||
a_mean_system_power.set_title(r"$\bar{P}_\mathrm{sys}/\Omega^2$")
|
||||
|
||||
(_, _, (c_work, data_work)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(-model.power(steady_idx=-2).value * model.Θ, 0, np.inf),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_work,
|
||||
)
|
||||
a_work.set_title(r"$W/\Omega$")
|
||||
|
||||
|
||||
plt.tight_layout()
|
||||
contours = [c_power, c_efficiency, c_work, c_mean_inter_power, c_mean_system_power]
|
||||
datas = [data_power, data_efficiency, data_work, data_mean_inter_power, data_mean_system_power]
|
||||
|
||||
for fig, contour in zip(figs, contours):
|
||||
fig.colorbar(contour)
|
||||
|
||||
fs.export_fig("coupling_speed_scan_power_contour", x_scaling=1, y_scaling=1, fig=f_power, data=data_power)
|
||||
fs.export_fig("coupling_speed_scan_work_contour", x_scaling=1, y_scaling=1, fig=f_work, data=data_work)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_efficiency_contour", x_scaling=1, y_scaling=1, fig=f_efficiency, data=data_efficiency
|
||||
)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_interpower_contour", x_scaling=1, y_scaling=1, fig=f_mean_inter_power, data=data_mean_inter_power
|
||||
)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_syspower_contour", x_scaling=1, y_scaling=1, fig=f_mean_system_power, data=data_mean_system_power
|
||||
)
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
[[file:./.ob-jupyter/67bf5c82306b318ce650433463e13e7dee354bd5.svg]]
|
||||
[[file:./.ob-jupyter/7e340c9e451d8dbd012b84be33801965f96122ac.svg]]
|
||||
[[file:./.ob-jupyter/32153d4bce153c132414c148d3e489130fdc87b3.svg]]
|
||||
[[file:./.ob-jupyter/6218def4404f7bf670a4d3e75c28d07ac6d9f101.svg]]
|
||||
[[file:./.ob-jupyter/806dbc342f97c822035fcf647f53b26b7cd846f0.svg]]
|
||||
:END:
|
||||
|
||||
#+begin_src jupyter-python
|
||||
f = plt.figure()
|
||||
|
|
@ -296,7 +372,7 @@ coupling-change/cycle time.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/f7ad9a0e9f9caefc557f1690582b5aa6abe22a01.svg]]
|
||||
[[file:./.ob-jupyter/43634f8b38594ef86dce9c67d4da46131bd0ad48.svg]]
|
||||
|
||||
|
||||
|
||||
|
|
|
|||
|
|
@ -58,21 +58,6 @@ aux.import_results(other_data_path="taurus/.data", other_results_path="taurus/re
|
|||
|
||||
ot.plot_energy(models[5])
|
||||
|
||||
for i in range(len(Θs)):
|
||||
fig, ax = plt.subplots()
|
||||
for model in models[len(δs) * i :len(δs) * (i+1)]:
|
||||
pu.plot_with_σ(model.t, model.system_energy(), ax=ax)
|
||||
|
||||
for model in models:
|
||||
plt.plot(model.t, abs(model.total_energy_from_power().value - model.total_energy().value))
|
||||
|
||||
#[model.efficiency(steady_idx=-2).value * 100 for model in models][10]
|
||||
models[10].strobe, models[1].strobe
|
||||
|
||||
models[10].system_energy().N
|
||||
|
||||
ot.plot_power_eff_convergence(models, 2)
|
||||
|
||||
f_power = plt.figure()
|
||||
a_power = f_power.add_subplot(1, 1, 1, projection="3d")
|
||||
f_work = plt.figure()
|
||||
|
|
@ -155,7 +140,7 @@ ot.plot_3d_heatmap(
|
|||
lambda model: model.Θ,
|
||||
ax=a_work,
|
||||
)
|
||||
a_work.set_zlabel(r"$-W$")
|
||||
a_work.set_zlabel(r"$W$")
|
||||
a_work.zaxis.labelpad = 8
|
||||
|
||||
|
||||
|
|
@ -173,6 +158,115 @@ fs.export_fig(
|
|||
"coupling_speed_scan_syspower", x_scaling=1, y_scaling=1, fig=f_mean_system_power
|
||||
)
|
||||
|
||||
f_mean_system_power = plt.figure()
|
||||
a_mean_system_power = f_mean_system_power.add_subplot(1, 1, 1)
|
||||
|
||||
(_, _, (c_mean_sytem_power, data_mean_system_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model:
|
||||
-ot.val_relative_to_steady(model, model.system_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_system_power,
|
||||
)
|
||||
a_mean_system_power.set_title(r"$\bar{P}_\mathrm{sys}/\Omega^2$")
|
||||
|
||||
f_power = plt.figure()
|
||||
a_power = f_power.add_subplot(1, 1, 1)
|
||||
f_work = plt.figure()
|
||||
a_work = f_work.add_subplot(1, 1, 1)
|
||||
f_efficiency = plt.figure()
|
||||
a_efficiency = f_efficiency.add_subplot(1, 1, 1)
|
||||
f_mean_inter_power = plt.figure()
|
||||
a_mean_inter_power = f_mean_inter_power.add_subplot(1, 1, 1)
|
||||
f_mean_system_power = plt.figure()
|
||||
a_mean_system_power = f_mean_system_power.add_subplot(1, 1, 1)
|
||||
|
||||
axs = [a_power, a_efficiency, a_work, a_mean_inter_power, a_mean_system_power]
|
||||
figs = [f_power, f_efficiency, f_work, f_mean_inter_power, f_mean_system_power]
|
||||
for ax in axs:
|
||||
ax.set_xlabel(r"$\delta$")
|
||||
ax.set_ylabel(r"$\Theta$")
|
||||
|
||||
|
||||
(_, _, (c_efficiency, data_efficiency)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(
|
||||
np.nan_to_num(model.efficiency(steady_idx=-2).value * 100), 0, np.inf
|
||||
),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_efficiency,
|
||||
)
|
||||
a_efficiency.set_title(r"$\eta$")
|
||||
|
||||
(_, _, (c_power, data_power)) =ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(-model.power(steady_idx=-2).value, 0, np.inf),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_power,
|
||||
)
|
||||
a_power.set_title(r"$\bar{P}/\Omega^2$")
|
||||
|
||||
(_, _, (c_mean_inter_power, data_mean_inter_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(
|
||||
ot.val_relative_to_steady(model, model.interaction_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
0,
|
||||
np.inf,
|
||||
),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_inter_power,
|
||||
)
|
||||
a_mean_inter_power.set_title(r"$-\bar{P}_\mathrm{int}/\Omega^2$")
|
||||
|
||||
(_, _, (c_mean_system_power, data_mean_system_power)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model:
|
||||
-ot.val_relative_to_steady(model, model.system_power().sum_baths(), 2)[
|
||||
1
|
||||
].mean.value,
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_mean_system_power,
|
||||
)
|
||||
a_mean_system_power.set_title(r"$\bar{P}_\mathrm{sys}/\Omega^2$")
|
||||
|
||||
(_, _, (c_work, data_work)) = ot.plot_contour(
|
||||
models,
|
||||
lambda model: np.clip(-model.power(steady_idx=-2).value * model.Θ, 0, np.inf),
|
||||
lambda model: model.δ[0],
|
||||
lambda model: model.Θ,
|
||||
ax=a_work,
|
||||
)
|
||||
a_work.set_title(r"$W/\Omega$")
|
||||
|
||||
|
||||
plt.tight_layout()
|
||||
contours = [c_power, c_efficiency, c_work, c_mean_inter_power, c_mean_system_power]
|
||||
datas = [data_power, data_efficiency, data_work, data_mean_inter_power, data_mean_system_power]
|
||||
|
||||
for fig, contour in zip(figs, contours):
|
||||
fig.colorbar(contour)
|
||||
|
||||
fs.export_fig("coupling_speed_scan_power_contour", x_scaling=1, y_scaling=1, fig=f_power, data=data_power)
|
||||
fs.export_fig("coupling_speed_scan_work_contour", x_scaling=1, y_scaling=1, fig=f_work, data=data_work)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_efficiency_contour", x_scaling=1, y_scaling=1, fig=f_efficiency, data=data_efficiency
|
||||
)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_interpower_contour", x_scaling=1, y_scaling=1, fig=f_mean_inter_power, data=data_mean_inter_power
|
||||
)
|
||||
fs.export_fig(
|
||||
"coupling_speed_scan_syspower_contour", x_scaling=1, y_scaling=1, fig=f_mean_system_power, data=data_mean_system_power
|
||||
)
|
||||
|
||||
f = plt.figure()
|
||||
a_power = f.add_subplot(121, projection="3d")
|
||||
a_efficiency = f.add_subplot(122, projection="3d")
|
||||
|
|
|
|||
Binary file not shown.
Binary file not shown.
Binary file not shown.
Binary file not shown.
Binary file not shown.
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12564
python/otto_motor/subprojects/cycle_shift/.dat.b/model_data.json
Normal file
12564
python/otto_motor/subprojects/cycle_shift/.dat.b/model_data.json
Normal file
File diff suppressed because it is too large
Load diff
|
|
@ -6043,7 +6043,7 @@ L -1180.963695 84.550875
|
|||
L -1181.571638 83.734756
|
||||
L -1182.179581 83.454065
|
||||
z
|
||||
" clip-path="url(#p874f95a634)" style="fill: #7fbee9; fill-opacity: 0.5; stroke: #7fbee9; stroke-opacity: 0.5; stroke-width: 0.24"/>
|
||||
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@ -69,7 +69,7 @@ We shift so that we just overlap with coupling/decoupling and one above.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/fc9a5d0d4ed29593313534e3d1a1a28da016afa8.svg]]
|
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[[file:./.ob-jupyter/3c4e1d96fdd126da5d4b38602db707635baad8ce.svg]]
|
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#+begin_src jupyter-python :tangle no
|
||||
#ot.plot_cycles(models, bath=0, legend=True)
|
||||
|
|
@ -93,7 +93,7 @@ We shift so that we just overlap with coupling/decoupling and one above.
|
|||
#+end_src
|
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#+RESULTS:
|
||||
[[file:./.ob-jupyter/ee72e133dfc7dfcd155f963b976b188805a1e49a.svg]]
|
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[[file:./.ob-jupyter/81bf7b0cd4af85e2d8893ef1bf1261a214135525.svg]]
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||||
** Integrate
|
||||
Here we integrate/simulate the models. This should be run on the
|
||||
|
|
@ -121,7 +121,7 @@ This plots the full energy overview for the baseline model.
|
|||
#+RESULTS:
|
||||
:RESULTS:
|
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: \(N=80000\)
|
||||
[[file:./.ob-jupyter/a679748c0a1c4e4f1c34301d35957a2a36fd91fc.svg]]
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[[file:./.ob-jupyter/73e9a2cd60b362f39b0b62a47056740f562e3d08.svg]]
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:END:
|
||||
|
||||
We would like to know how close all of this comes to the thermal states.
|
||||
|
|
@ -160,7 +160,6 @@ We would like to know how close all of this comes to the thermal states.
|
|||
#+end_src
|
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|
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#+RESULTS:
|
||||
:RESULTS:
|
||||
#+begin_example
|
||||
[[0.11920292 0. ]
|
||||
[0. 0.88079708]]
|
||||
|
|
@ -177,8 +176,6 @@ We would like to know how close all of this comes to the thermal states.
|
|||
/nix/store/fai1b55231rnk4jyj0kjicdnqcgdf9ph-python3-3.9.15-env/lib/python3.9/site-packages/matplotlib/axes/_axes.py:5346: ComplexWarning: Casting complex values to real discards the imaginary part
|
||||
pts[N+2:, 1] = dep2slice[::-1]
|
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#+end_example
|
||||
[[file:./.ob-jupyter/96f49e4d6c26be8d062e45ea53198b6232a05e9f.svg]]
|
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:END:
|
||||
|
||||
Plotting the pauli matrix expectation values, we can see that the
|
||||
dynamics only take place on the z-axis. This is addressed in [[id:9d7a11f2-f479-4e95-8775-31050bcc4fb7][Off-Axis Hamiltonian]]
|
||||
|
|
@ -188,7 +185,7 @@ dynamics only take place on the z-axis. This is addressed in [[id:9d7a11f2-f479-
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/746d8e3986e828734631ca1ab8a8bce243963588.svg]]
|
||||
[[file:./.ob-jupyter/a645250e5f7a8890257674fe5de32b09d9de78f1.svg]]
|
||||
|
||||
Let us plot an overview of the work done by system and interaction
|
||||
modulation over a cycle for the baseline model.
|
||||
|
|
@ -198,7 +195,7 @@ modulation over a cycle for the baseline model.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/e05d323e86738a3362e6c70adc16bd5d940e5cdd.svg]]
|
||||
[[file:./.ob-jupyter/888e4e87b2f952b2d1866055b087a2d0bfe38ed0.svg]]
|
||||
|
||||
*** Shifted Models
|
||||
Let us print the power output (relative to the baseline = unshifted model) and efficiency.
|
||||
|
|
@ -209,17 +206,17 @@ Let us print the power output (relative to the baseline = unshifted model) and e
|
|||
|
||||
#+RESULTS:
|
||||
#+begin_example
|
||||
-2.77597511693978 -2.4772877227717958
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||||
-2.0434846540636498 -1.6243768550730728
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0.5710213861808199 0.19310160522534914
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1.0 0.3002164459369506
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1.1580729241081245 0.3201551362641393
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1.621073860181052 0.32914493962691976
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1.676329717306901 0.3155858623648209
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1.6056907132267833 0.29627949690062266
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1.4297898620293028 0.264279816138587
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0.7161356715968495 0.13903993767016806
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-1.2535087048383218 -0.29154092061712156
|
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-2.77597511693978 -2.4772877227717958
|
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-2.0434846540636498 -1.6243768550730728
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0.5710213861808199 0.19310160522534914
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1.0 0.3002164459369506
|
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1.1580729241081245 0.3201551362641393
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1.621073860181052 0.32914493962691976
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1.676329717306901 0.3155858623648209
|
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1.6056907132267833 0.29627949690062266
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1.4297898620293028 0.264279816138587
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||||
0.7161356715968495 0.13903993767016806
|
||||
-1.2535087048383218 -0.29154092061712156
|
||||
#+end_example
|
||||
|
||||
|
||||
|
|
@ -231,7 +228,7 @@ size to check convergence.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/c671a1b46de1f5b65905925fb69604e13a924e19.svg]]
|
||||
[[file:./.ob-jupyter/8d9b7d2fcd5ef897070660fa264fd9e904a916ea.svg]]
|
||||
|
||||
We see that we get a pretty good picture after about 30k-40k samples.
|
||||
|
||||
|
|
@ -242,7 +239,7 @@ This is an overview over powers and the efficiency.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/c134d0ea85b5900cc5fc809ee73e68d332d429d6.svg]]
|
||||
[[file:./.ob-jupyter/95ce996f5adf865114a7efc488992da2993495a8.svg]]
|
||||
|
||||
The best shift:
|
||||
#+begin_src jupyter-python
|
||||
|
|
@ -263,7 +260,7 @@ and the best shift model.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/f7afc8eb774b72b6f9a3080a0884226164759391.svg]]
|
||||
[[file:./.ob-jupyter/1b65cbe8a112cceb40aa0440d33ed40dca30dcf1.svg]]
|
||||
|
||||
|
||||
Let us plot the interaction power in the steady state for baseline and
|
||||
|
|
@ -317,7 +314,7 @@ best-shift. We have to shift the time to make them overlap correctly.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/3e6540b6d222f368a38f57540b7c70c5758f5b99.svg]]
|
||||
[[file:./.ob-jupyter/ebdd9c91ce756ae30681a68a43f439514a96bf8d.svg]]
|
||||
|
||||
|
||||
Let us zoom in on the cold bath decoupling process to understnad this better.
|
||||
|
|
@ -359,7 +356,7 @@ Let us zoom in on the cold bath decoupling process to understnad this better.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/2f00757c397d5533da72e20f6a650af459861c22.svg]]
|
||||
[[file:./.ob-jupyter/15e1e2b441e6a10d9b69f585ff691d7e54d0320d.svg]]
|
||||
|
||||
How does this look like for the baseline?
|
||||
#+begin_src jupyter-python
|
||||
|
|
@ -401,7 +398,7 @@ How does this look like for the baseline?
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/c5cda1720747169d3572e9b38b2946cb4eb1b62e.svg]]
|
||||
[[file:./.ob-jupyter/392899a8a7f82eda25a92fad0cf029862311594f.svg]]
|
||||
|
||||
|
||||
* Slower switching
|
||||
|
|
@ -441,8 +438,8 @@ switch slower.
|
|||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
: <matplotlib.legend.Legend at 0x7f5da18c38e0>
|
||||
[[file:./.ob-jupyter/b77a8b40f7c3265be026db00a76524da7bff95c4.svg]]
|
||||
: <matplotlib.legend.Legend at 0x7f2401d01d30>
|
||||
[[file:./.ob-jupyter/ab754a91833374afaab5ef6e50c895e6d05f9f58.svg]]
|
||||
:END:
|
||||
|
||||
|
||||
|
|
@ -468,17 +465,17 @@ Let us look at power and efficiency.
|
|||
|
||||
#+RESULTS:
|
||||
#+begin_example
|
||||
-0.18 0.18 80000 -0.7534604455561659 -108.77944601456684 (-0.6547883379568094, 0.4330061221888589)
|
||||
-0.12 0.18 80000 0.5591648896822077 -14.974955411404467 (0.28325656807481425, 0.4330061221888589)
|
||||
-0.06 0.18 80000 0.9985149794296736 0.0037407432686098474 (0.433043529621545, 0.4330061221888589)
|
||||
0.0 0.18 80000 1.0 0.0 (0.4330061221888589, 0.4330061221888589)
|
||||
0.06 0.18 80000 0.991206944683175 0.23007686496274715 (0.4353068908384864, 0.4330061221888589)
|
||||
0.12 0.18 80000 1.1339755806282883 0.3265587668820624 (0.43627170985767955, 0.4330061221888589)
|
||||
0.18 0.18 80000 1.297675283650504 -2.9821368425732797 (0.4031847537631261, 0.4330061221888589)
|
||||
0.24 0.18 80000 1.2031272812376834 -7.638926235390614 (0.3566168598349528, 0.4330061221888589)
|
||||
0.3 0.18 80000 0.7381994151953918 -20.86521478070438 (0.22435397438181512, 0.4330061221888589)
|
||||
0.36 0.18 80000 -0.45819153140116126 -60.284418918547836 (-0.16983806699661946, 0.4330061221888589)
|
||||
0.42 0.18 80000 -1.4846084056353754 -118.88415735590576 (-0.7558354513701987, 0.4330061221888589)
|
||||
-0.18 0.18 80000 -0.7534604455561659 -108.77944601456684 (-0.6547883379568094, 0.4330061221888589)
|
||||
-0.12 0.18 80000 0.5591648896822077 -14.974955411404467 (0.28325656807481425, 0.4330061221888589)
|
||||
-0.06 0.18 80000 0.9985149794296736 0.0037407432686098474 (0.433043529621545, 0.4330061221888589)
|
||||
0.0 0.18 80000 1.0 0.0 (0.4330061221888589, 0.4330061221888589)
|
||||
0.06 0.18 80000 0.991206944683175 0.23007686496274715 (0.4353068908384864, 0.4330061221888589)
|
||||
0.12 0.18 80000 1.1339755806282883 0.3265587668820624 (0.43627170985767955, 0.4330061221888589)
|
||||
0.18 0.18 80000 1.297675283650504 -2.9821368425732797 (0.4031847537631261, 0.4330061221888589)
|
||||
0.24 0.18 80000 1.2031272812376834 -7.638926235390614 (0.3566168598349528, 0.4330061221888589)
|
||||
0.3 0.18 80000 0.7381994151953918 -20.86521478070438 (0.22435397438181512, 0.4330061221888589)
|
||||
0.36 0.18 80000 -0.45819153140116126 -60.284418918547836 (-0.16983806699661946, 0.4330061221888589)
|
||||
0.42 0.18 80000 -1.4846084056353754 -118.88415735590576 (-0.7558354513701987, 0.4330061221888589)
|
||||
#+end_example
|
||||
|
||||
Here, we contrast the slow/fast coupling modulation protocols.
|
||||
|
|
@ -496,7 +493,7 @@ Here, we contrast the slow/fast coupling modulation protocols.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/d874adc97bcc335737347c1205a48c7b39561198.svg]]
|
||||
[[file:./.ob-jupyter/2da75cadbb1995855015de60aeb90c920565d142.svg]]
|
||||
|
||||
Aho! The trick is just to slow down the coupling switching.
|
||||
|
||||
|
|
@ -988,7 +985,7 @@ hamiltonian.
|
|||
|
||||
#+begin_src jupyter-python :tangle tangle/rot.py
|
||||
rot_models = []
|
||||
weights = [.5]
|
||||
weights = [.3, .5]
|
||||
for weight in weights:
|
||||
off_ax = sc.make_model(0, 0)
|
||||
off_ax.H_bias = ConstantMatrix(weight / 2 * qt.sigmax().full())
|
||||
|
|
@ -1010,10 +1007,20 @@ hamiltonian.
|
|||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
| <matplotlib.lines.Line2D | at | 0x7f36470cdd00> |
|
||||
[[file:./.ob-jupyter/d5d7c229833877657c2abc95a30a085919c05d40.svg]]
|
||||
| <matplotlib.lines.Line2D | at | 0x7f00c44f6cd0> |
|
||||
[[file:./.ob-jupyter/7a6d38b0d03238b0d00694a60068273f8382ac8f.svg]]
|
||||
:END:
|
||||
|
||||
#+begin_src jupyter-python
|
||||
for model in rot_models:
|
||||
print(model.energy_gaps[1] - model.energy_gaps[0])
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
: 0.9783441907246133
|
||||
: 0.9435188240589354
|
||||
|
||||
|
||||
** Integration
|
||||
#+begin_src jupyter-python :tangle tangle/rot.py
|
||||
ot.integrate_online_multi(rot_models, 80_000, increment=10_000, analyze_kwargs=dict(every=10_000))
|
||||
|
|
@ -1023,105 +1030,6 @@ hamiltonian.
|
|||
aux.import_results(other_data_path="taurus/.data", other_results_path="taurus/results", models_to_import=rot_models)
|
||||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
#+begin_example
|
||||
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||||
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||||
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||||
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||||
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||||
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||||
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||||
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|
||||
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||||
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||||
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||||
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||||
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||||
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|
||||
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||||
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||||
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||||
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|
||||
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|
||||
[INFO root 466059] Skipping ca94f36cbacd1b29d6e4f3cf384624ef0f4930ef3b0f12b09179efb17e327454.
|
||||
[WARNING root 466059] Importing taurus/.data/e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76/_e/e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_ef101bcb3b36a4bf1fb509507482e323_1.h5 to .data/e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76/_e/e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_ef101bcb3b36a4bf1fb509507482e323_1.h5.
|
||||
[WARNING root 466059] The model description is 'Classic Cycle'.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_30000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_50000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_80000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_70000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_20000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_60000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_40000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/flow_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_10000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_80000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_10000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_70000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_60000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_20000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_50000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_30000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_40000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_30000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_20000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_60000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_10000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_70000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_50000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_40000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/interaction_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_80000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_50000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_30000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_10000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_60000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_20000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_80000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_40000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_70000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_80000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_20000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_40000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_70000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_50000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_30000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_10000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76_60000.npz.
|
||||
[WARNING root 466059] Importing taurus/results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz to results/system_power_e9ff5f43faa62deec9fddc939d63ab5742569d6ee6801a149718b670e1636e76.npz.
|
||||
#+end_example
|
||||
|
||||
** Analysis
|
||||
#+begin_src jupyter-python
|
||||
for (i, model), weight in zip(enumerate(rot_models), weights):
|
||||
|
|
@ -1133,7 +1041,10 @@ hamiltonian.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/fc25ed2715cfa569942ee1d2f49229335cb7b476.svg]]
|
||||
:RESULTS:
|
||||
[[file:./.ob-jupyter/e47b10f766f959556b716834bb8b04f7fad6f9aa.svg]]
|
||||
[[file:./.ob-jupyter/e08e289587db6444af876ccf358a43308eb79d39.svg]]
|
||||
:END:
|
||||
|
||||
#+begin_src jupyter-python
|
||||
for (i, model), weight in zip(enumerate(rot_models), weights):
|
||||
|
|
@ -1143,7 +1054,10 @@ hamiltonian.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/dadb90f0626b8b89f51b77552f2cc31f2411a0d7.svg]]
|
||||
:RESULTS:
|
||||
[[file:./.ob-jupyter/46aebae6079822280c7af62e1179c5eea48c07cf.svg]]
|
||||
[[file:./.ob-jupyter/d64002e262380b8ac3289adad61486eafb8743fe.svg]]
|
||||
:END:
|
||||
|
||||
|
||||
#+begin_src jupyter-python
|
||||
|
|
@ -1152,7 +1066,8 @@ hamiltonian.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
: 0.9891011003410791 0.9485880353543075
|
||||
: 0.9291297056238266 0.9345445495028932
|
||||
: 0.783979849642736 0.804865129162892
|
||||
|
||||
#+begin_src jupyter-python
|
||||
fig, axs = plt.subplots(ncols=2)
|
||||
|
|
@ -1162,7 +1077,7 @@ hamiltonian.
|
|||
ax.set_xlabel(r"$\tau$")
|
||||
ax.set_ylabel(r"$\Delta X$")
|
||||
|
||||
for (i, model) in enumerate([*rot_models, baseline]):
|
||||
for (i, model) in enumerate([*rot_models[1:], baseline]):
|
||||
for j, (val, label) in enumerate(zip([
|
||||
model.total_energy_from_power(),
|
||||
model.system_energy(),
|
||||
|
|
@ -1180,4 +1095,4 @@ hamiltonian.
|
|||
#+end_src
|
||||
|
||||
#+RESULTS:
|
||||
[[file:./.ob-jupyter/9ea7484406e68614657b87986a4fd9599d9d289a.svg]]
|
||||
[[file:./.ob-jupyter/634ba0cb457f6145c9e22d45d6b78f27ab630a6d.svg]]
|
||||
|
|
|
|||
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Loading…
Add table
Reference in a new issue