Welcome to QuCumber’s documentation!

Installation

QuCumber only supports Python 3, not Python 2. If you are using Python 2, please update! You will also want to install the following packages, if you have not already.

  1. Pytorch v0.4.1 (https://pytorch.org/)
  2. tqdm (https://github.com/tqdm/tqdm)

Github

Navigate to the qucumber page on github (https://github.com/PIQuIL/QuCumber) and clone the repository by typing:

git clone https://github.com/PIQuIL/QuCumber.git

Navigate to the main directory and type:

python setup.py install

Windows

Navigate to the directory (through command prompt) where pip.exe is installed (usually C:\Python\Scripts\pip.exe) and type:

pip.exe install qucumber

Linux / MacOS

Open up a terminal, then type:

pip install qucumber

Theory

For a basic introduction to Restricted Boltzmann Machines, click here.

Download the tutorials

Once you have installed QuCumber, we recommend going through our tutorial that is divided into two parts.

  1. Training a wave function to reconstruct a positive-real wave function (i.e. no phase) from a transverse-field Ising model (TFIM) and then generating new data.
  2. Training an wave function to reconstruct a complex wave function (i.e. with a phase) from a simple two qubit random state and then generating new data.

We have made interactive python notebooks that can be downloaded (along with the data required) here. Note that the linked examples are from the most recent stable release (relative to the version of the docs you’re currently viewing), and may not match the examples shown in the following pages. It is recommended that you refer to documentation for the latest stable release: https://qucumber.readthedocs.io/en/stable/.

If you wish to simply view the static, non-interactive notebooks, continue to the next page of the documentation.

Alternatively, you can view interactive notebooks online at: BinderBadge, though they may be slow.

This is a static, non-editable tutorial.

We recommend you install QuCumber if you want to run the examples locally. You can then get an archive file containing the examples from the relevant release here. Alternatively, you can launch an interactive online version, though it may be a bit slow: Binder badge

Reconstruction of a positive-real wavefunction

In this tutorial, a walkthrough of how to reconstruct a positive-real wavefunction via training a Restricted Boltzmann Machine (RBM), the neural network behind qucumber, will be presented. The data used for training will be \sigma^{z} measurements from a one-dimensional transverse-field Ising model (TFIM) with 10 sites at its critical point.

Transverse-field Ising model

The example dataset, located in tfim1d_data.txt, comprises of 10,000 \sigma^{z} measurements from a one-dimensional transverse-field Ising model (TFIM) with 10 sites at its critical point. The Hamiltonian for the transverse-field Ising model (TFIM) is given by

\begin{equation} \mathcal{H} = -J\sum_i \sigma^z_i \sigma^z_{i+1} - h \sum_i \sigma^x_i \end{equation}

where \sigma^{z}_i is the conventional spin-1/2 Pauli operator on site i. At the critical point, J=h=1. As per convention, spins are represented in binary notation with zero and one denoting spin-down and spin-up, respectively.

Using qucumber to reconstruct the wavefunction

Imports

To begin the tutorial, first import the required Python packages.

[1]:

import numpy as np
import matplotlib.pyplot as plt

from qucumber.nn_states import PositiveWaveFunction
from qucumber.callbacks import MetricEvaluator

import qucumber.utils.training_statistics as ts
import qucumber.utils.data as data

The Python class PositiveWaveFunction contains generic properties of a RBM meant to reconstruct a positive-real wavefunction, the most notable one being the gradient function required for stochastic gradient descent.

To instantiate a PositiveWaveFunction object, one needs to specify the number of visible and hidden units in the RBM. The number of visible units, num_visible, is given by the size of the physical system, i.e. the number of spins or qubits (10 in this case), while the number of hidden units, num_hidden, can be varied to change the expressiveness of the neural network.

Note: The optimal num_hidden : num_visible ratio will depend on the system. For the TFIM, having this ratio be equal to 1 leads to good results with reasonable computational effort.

Training

To evaluate the training in real time, the fidelity between the true ground-state wavefunction of the system and the wavefunction that qucumber reconstructs, \vert\langle\psi\vert\psi_{RBM}\rangle\vert^2, will be calculated along with the Kullback-Leibler (KL) divergence (the RBM’s cost function). It will also be shown that any custom function can be used to evaluate the training.

First, the training data and the true wavefunction of this system must be loaded using the data utility.

[2]:

psi_path = "tfim1d_psi.txt"
train_path = "tfim1d_data.txt"
train_data, true_psi = data.load_data(train_path, psi_path)

As previously mentioned, to instantiate a PositiveWaveFunction object, one needs to specify the number of visible and hidden units in the RBM. These two quantities equal will be kept equal.

[3]:

nv = train_data.shape[-1]
nh = nv

nn_state = PositiveWaveFunction(num_visible=nv, num_hidden=nh)
# nn_state = PositiveWaveFunction(num_visible=nv, num_hidden=nh, gpu = False)

By default, qucumber will attempt to run on a GPU if one is available (if one is not available, qucumber will default to CPU). If one wishes to run qucumber on a CPU, add the flag “gpu = False” in the PositiveWaveFunction object instantiation (i.e. uncomment the line above).

Now the hyperparameters of the training process can be specified.

  1. epochs: the total number of training cycles that will be performed (default = 100)

  2. pos_batch_size: the number of data points used in the positive phase of the gradient (default = 100)

  3. neg_batch_size: the number of data points used in the negative phase of the gradient (default = pos_batch_size)

  4. k: the number of contrastive divergence steps (default = 1)

  5. lr: the learning rate (default = 0.001)

    Note: For more information on the hyperparameters above, it is strongly encouraged that the user to read through the brief, but thorough theory document on RBMs located in the qucumber documentation. One does not have to specify these hyperparameters, as their default values will be used without the user overwriting them. It is recommended to keep with the default values until the user has a stronger grasp on what these hyperparameters mean. The quality and the computational efficiency of the training will highly depend on the choice of hyperparameters. As such, playing around with the hyperparameters is almost always necessary.

For the TFIM with 10 sites, the following hyperparameters give excellent results.

[4]:

epochs = 500
pbs = 100  # pos_batch_size
nbs = 200  # neg_batch_size
lr = 0.01
k = 10

For evaluating the training in real time, the MetricEvaluator will be called in order to calculate the training evaluators every 100 epochs. The MetricEvaluator requires the following arguments.

  1. log_every: the frequency of the training evaluators being calculated is controlled by the log_every argument (e.g. log_every = 200 means that the MetricEvaluator will update the user every 200 epochs)
  2. A dictionary of functions you would like to reference to evaluate the training (arguments required for these functions are keyword arguments placed after the dictionary)

The following additional arguments are needed to calculate the fidelity and KL divergence in the training_statistics utility.

  • target_psi: the true wavefunction of the system
  • space: the hilbert space of the system

The training evaluators can be printed out via the verbose=True statement.

Although the fidelity and KL divergence are excellent training evaluators, they are not practical to calculate in most cases; the user may not have access to the target wavefunction of the system, nor may generating the hilbert space of the system be computationally feasible. However, evaluating the training in real time is extremely convenient.

Any custom function that the user would like to use to evaluate the training can be given to the MetricEvaluator, thus avoiding having to calculate fidelity and/or KL divergence. Any custom function given to MetricEvaluator must take the neural-network state (in this case, the PositiveWaveFunction object) and keyword arguments. As an example, the function to be passed to the MetricEvaluator will be the fifth coefficient of the reconstructed wavefunction multiplied by a parameter, A.

[5]:

def psi_coefficient(nn_state, space, A, **kwargs):
    norm = nn_state.compute_normalization(space).sqrt_()
    return A * nn_state.psi(space)[0][4] / norm

Now the hilbert space of the system can be generated for the fidelity and KL divergence and the dictionary of functions the user would like to compute every “log_every” epochs can be given to the MetricEvaluator.

[6]:

log_every = 10
space = nn_state.generate_hilbert_space(nv)

Now the training can begin. The PositiveWaveFunction object has a property called fit which takes care of this. MetricEvaluator must be passed to the fit function in a list (callbacks).

[7]:

callbacks = [
    MetricEvaluator(
        log_every,
        {"Fidelity": ts.fidelity, "KL": ts.KL, "A_Ψrbm_5": psi_coefficient},
        target_psi=true_psi,
        verbose=True,
        space=space,
        A=3.,
    )
]

nn_state.fit(
    train_data,
    epochs=epochs,
    pos_batch_size=pbs,
    neg_batch_size=nbs,
    lr=lr,
    k=k,
    callbacks=callbacks,
)
# nn_state.fit(train_data, callbacks=callbacks)

Epoch: 10       Fidelity = 0.524441     KL = 1.311481   A_Ψrbm_5 = 0.102333
Epoch: 20       Fidelity = 0.627167     KL = 0.887134   A_Ψrbm_5 = 0.151670
Epoch: 30       Fidelity = 0.733927     KL = 0.582645   A_Ψrbm_5 = 0.194329
Epoch: 40       Fidelity = 0.794879     KL = 0.445741   A_Ψrbm_5 = 0.221883
Epoch: 50       Fidelity = 0.829248     KL = 0.363647   A_Ψrbm_5 = 0.232239
Epoch: 60       Fidelity = 0.860589     KL = 0.287518   A_Ψrbm_5 = 0.241004
Epoch: 70       Fidelity = 0.886160     KL = 0.231527   A_Ψrbm_5 = 0.244122
Epoch: 80       Fidelity = 0.902777     KL = 0.196992   A_Ψrbm_5 = 0.234641
Epoch: 90       Fidelity = 0.914448     KL = 0.174226   A_Ψrbm_5 = 0.231594
Epoch: 100      Fidelity = 0.923648     KL = 0.156510   A_Ψrbm_5 = 0.234137
Epoch: 110      Fidelity = 0.929855     KL = 0.142626   A_Ψrbm_5 = 0.220506
Epoch: 120      Fidelity = 0.937082     KL = 0.127953   A_Ψrbm_5 = 0.228048
Epoch: 130      Fidelity = 0.943320     KL = 0.114683   A_Ψrbm_5 = 0.225533
Epoch: 140      Fidelity = 0.948913     KL = 0.102805   A_Ψrbm_5 = 0.220003
Epoch: 150      Fidelity = 0.953720     KL = 0.092966   A_Ψrbm_5 = 0.219529
Epoch: 160      Fidelity = 0.957696     KL = 0.085269   A_Ψrbm_5 = 0.219721
Epoch: 170      Fidelity = 0.960716     KL = 0.079273   A_Ψrbm_5 = 0.215919
Epoch: 180      Fidelity = 0.963032     KL = 0.075418   A_Ψrbm_5 = 0.219223
Epoch: 190      Fidelity = 0.965285     KL = 0.071062   A_Ψrbm_5 = 0.217072
Epoch: 200      Fidelity = 0.966294     KL = 0.069517   A_Ψrbm_5 = 0.218791
Epoch: 210      Fidelity = 0.968279     KL = 0.065436   A_Ψrbm_5 = 0.214237
Epoch: 220      Fidelity = 0.969002     KL = 0.063958   A_Ψrbm_5 = 0.208316
Epoch: 230      Fidelity = 0.970735     KL = 0.060499   A_Ψrbm_5 = 0.211827
Epoch: 240      Fidelity = 0.971954     KL = 0.058173   A_Ψrbm_5 = 0.213458
Epoch: 250      Fidelity = 0.972797     KL = 0.056356   A_Ψrbm_5 = 0.216414
Epoch: 260      Fidelity = 0.973940     KL = 0.054098   A_Ψrbm_5 = 0.219072
Epoch: 270      Fidelity = 0.975173     KL = 0.051311   A_Ψrbm_5 = 0.213439
Epoch: 280      Fidelity = 0.976146     KL = 0.049353   A_Ψrbm_5 = 0.214791
Epoch: 290      Fidelity = 0.977626     KL = 0.046184   A_Ψrbm_5 = 0.215294
Epoch: 300      Fidelity = 0.978880     KL = 0.043539   A_Ψrbm_5 = 0.215247
Epoch: 310      Fidelity = 0.979931     KL = 0.041293   A_Ψrbm_5 = 0.211467
Epoch: 320      Fidelity = 0.981140     KL = 0.038849   A_Ψrbm_5 = 0.213601
Epoch: 330      Fidelity = 0.982012     KL = 0.036976   A_Ψrbm_5 = 0.216033
Epoch: 340      Fidelity = 0.982764     KL = 0.035460   A_Ψrbm_5 = 0.217036
Epoch: 350      Fidelity = 0.983499     KL = 0.033983   A_Ψrbm_5 = 0.208566
Epoch: 360      Fidelity = 0.984789     KL = 0.031407   A_Ψrbm_5 = 0.218186
Epoch: 370      Fidelity = 0.985142     KL = 0.030643   A_Ψrbm_5 = 0.215245
Epoch: 380      Fidelity = 0.985985     KL = 0.028931   A_Ψrbm_5 = 0.217562
Epoch: 390      Fidelity = 0.986345     KL = 0.028262   A_Ψrbm_5 = 0.217989
Epoch: 400      Fidelity = 0.986798     KL = 0.027449   A_Ψrbm_5 = 0.215068
Epoch: 410      Fidelity = 0.987459     KL = 0.026076   A_Ψrbm_5 = 0.220650
Epoch: 420      Fidelity = 0.987785     KL = 0.025427   A_Ψrbm_5 = 0.220902
Epoch: 430      Fidelity = 0.988085     KL = 0.024916   A_Ψrbm_5 = 0.217657
Epoch: 440      Fidelity = 0.988270     KL = 0.024565   A_Ψrbm_5 = 0.218701
Epoch: 450      Fidelity = 0.988164     KL = 0.024811   A_Ψrbm_5 = 0.222711
Epoch: 460      Fidelity = 0.988564     KL = 0.024018   A_Ψrbm_5 = 0.212042
Epoch: 470      Fidelity = 0.988859     KL = 0.023432   A_Ψrbm_5 = 0.221610
Epoch: 480      Fidelity = 0.989148     KL = 0.022804   A_Ψrbm_5 = 0.224286
Epoch: 490      Fidelity = 0.989477     KL = 0.022194   A_Ψrbm_5 = 0.223508
Epoch: 500      Fidelity = 0.989738     KL = 0.021626   A_Ψrbm_5 = 0.223838

All of these training evaluators can be accessed after the training has completed, as well. The code below shows this, along with plots of each training evaluator versus the training cycle number (epoch).

[8]:

fidelities = callbacks[0].Fidelity
KLs = callbacks[0].KL
coeffs = callbacks[0].A_Ψrbm_5
# Please note that the key given to the *MetricEvaluator* must be what comes after callbacks[0].
epoch = np.arange(log_every, epochs + 1, log_every)

[9]:

# Some parameters to make the plots look nice
params = {'text.usetex': True,
            'font.family': 'serif',
            'legend.fontsize': 14,
            'figure.figsize': (10, 3),
            'axes.labelsize': 16,
            'xtick.labelsize':14,
            'ytick.labelsize':14,
            'lines.linewidth':2,
            'lines.markeredgewidth': 0.8,
            'lines.markersize': 5,
            'lines.marker': "o",
            "patch.edgecolor": "black"
         }
plt.rcParams.update(params)
plt.style.use('seaborn-deep')

[10]:

# Plotting
fig, axs = plt.subplots(nrows=1, ncols=3, figsize=(14, 3))
ax = axs[0]
ax.plot(epoch, fidelities, "o", color = "C0", markeredgecolor="black")
ax.set_ylabel(r'Fidelity')
ax.set_xlabel(r'Epoch')

ax = axs[1]
ax.plot(epoch, KLs, "o", color = "C1", markeredgecolor="black")
ax.set_ylabel(r'KL Divergence')
ax.set_xlabel(r'Epoch')

ax = axs[2]
ax.plot(epoch, coeffs, "o", color = "C2", markeredgecolor="black")
ax.set_ylabel(r'$A\psi_{RBM}[5]$')
ax.set_xlabel(r'Epoch')

plt.tight_layout()
plt.savefig("fid_KL.pdf")
plt.show()
_images/_examples_Tutorial1_TrainPosRealWaveFunction_tutorial_quantum_ising_17_0.png

It should be noted that one could have just ran nn_state.fit(train_samples) and just used the default hyperparameters and no training evaluators.

To demonstrate how important it is to find the optimal hyperparameters for a certain system, restart this notebook and comment out the original fit statement and uncomment the one below. The default hyperparameters will be used instead. Using the non-default hyperparameters yielded a fidelity of approximately 0.994, while the default hyperparameters yielded a fidelity of approximately 0.523!

The RBM’s parameters will also be saved for future use in other tutorials. They can be saved to a pickle file with the name “saved_params.pt” with the code below.

[11]:

nn_state.save("saved_params.pt")

This saves the weights, visible biases and hidden biases as torch tensors with the following keys: “weights”, “visible_bias”, “hidden_bias”.

This is a static, non-editable tutorial.

We recommend you install QuCumber if you want to run the examples locally. You can then get an archive file containing the examples from the relevant release here. Alternatively, you can launch an interactive online version, though it may be a bit slow: Binder badge

Reconstruction of a complex wavefunction

In this tutorial, a walkthrough of how to reconstruct a complex wavefunction via training a Restricted Boltzmann Machine (RBM), the neural network behind qucumber, will be presented.

The wavefunction to be reconstructed

The simple wavefunction below describing two qubits (coefficients stored in qubits_psi.txt) will be reconstructed.

\begin{equation} \vert\psi \rangle = \alpha \vert00\rangle + \beta \vert 01\rangle + \gamma \vert10\rangle + \delta \vert11\rangle \end{equation}

where the exact values of \alpha, \beta, \gamma and \delta used for this tutorial are

\begin{align} \alpha & = 0.2861 + 0.0539 i \\ \beta & = 0.3687 - 0.3023 i \\ \gamma & = -0.1672 - 0.3529 i \\ \delta & = -0.5659 - 0.4639 i. \end{align}

The example dataset, qubits_train.txt, comprises of 500 \sigma measurements made in various bases (X, Y and Z). A corresponding file containing the bases for each data point in qubits_train.txt, qubits_train_bases.txt, is also required. As per convention, spins are represented in binary notation with zero and one denoting spin-down and spin-up, respectively.

Using qucumber to reconstruct the wavefunction

Imports

To begin the tutorial, first import the required Python packages.

[1]:

import numpy as np
import torch
import matplotlib.pyplot as plt

from qucumber.nn_states import ComplexWaveFunction

from qucumber.callbacks import MetricEvaluator

import qucumber.utils.unitaries as unitaries
import qucumber.utils.cplx as cplx

import qucumber.utils.training_statistics as ts
import qucumber.utils.data as data

The Python class ComplexWaveFunction contains generic properties of a RBM meant to reconstruct a complex wavefunction, the most notable one being the gradient function required for stochastic gradient descent.

To instantiate a ComplexWaveFunction object, one needs to specify the number of visible and hidden units in the RBM. The number of visible units, num_visible, is given by the size of the physical system, i.e. the number of spins or qubits (2 in this case), while the number of hidden units, num_hidden, can be varied to change the expressiveness of the neural network.

Note: The optimal num_hidden : num_visible ratio will depend on the system. For the two-qubit wavefunction described above, good results are yielded when this ratio is 1.

On top of needing the number of visible and hidden units, a ComplexWaveFunction object requires the user to input a dictionary containing the unitary operators (2x2) that will be used to rotate the qubits in and out of the computational basis, Z, during the training process. The unitaries utility will take care of creating this dictionary.

The MetricEvaluator class and training_statistics utility are built-in amenities that will allow the user to evaluate the training in real time.

Lastly, the cplx utility allows qucumber to be able to handle complex numbers. Currently, Pytorch does not support complex numbers.

Training

To evaluate the training in real time, the fidelity between the true wavefunction of the system and the wavefunction that qucumber reconstructs, \vert\langle\psi\vert\psi_{RBM}\rangle\vert^2, will be calculated along with the Kullback-Leibler (KL) divergence (the RBM’s cost function). First, the training data and the true wavefunction of this system need to be loaded using the data utility.

[2]:

train_path = "qubits_train.txt"
train_bases_path = "qubits_train_bases.txt"
psi_path = "qubits_psi.txt"
bases_path = "qubits_bases.txt"

train_samples, true_psi, train_bases, bases = data.load_data(
    train_path, psi_path, train_bases_path, bases_path
)

The file qubits_bases.txt contains every unique basis in the qubits_train_bases.txt file. Calculation of the full KL divergence in every basis requires the user to specify each unique basis.

As previouosly mentioned, a ComplexWaveFunction object requires a dictionary that contains the unitariy operators that will be used to rotate the qubits in and out of the computational basis, Z, during the training process. In the case of the provided dataset, the unitaries required are the well-known H, and K gates. The dictionary needed can be created with the following command.

[3]:

unitary_dict = unitaries.create_dict()
# unitary_dict = unitaries.create_dict(unitary_name=torch.tensor([[real part],
#                                                                 [imaginary part]],
#                                                                 dtype=torch.double)

If the user wishes to add their own unitary operators from their experiment to unitary_dict, uncomment the block above. When unitaries.create_dict() is called, it will contain the identity and the H and K gates by default with the keys “Z”, “X” and “Y”, respectively.

The number of visible units in the RBM is equal to the number of qubits. The number of hidden units will also be taken to be the number of visible units.

[4]:

nv = train_samples.shape[-1]
nh = nv

nn_state = ComplexWaveFunction(
    num_visible=nv, num_hidden=nh, unitary_dict=unitary_dict, gpu=False
)
# nn_state = ComplexWaveFunction(num_visible=nv, num_hidden=nh, unitary_dict=unitary_dict)

By default, qucumber will attempt to run on a GPU if one is available (if one is not available, qucumber will default to CPU). If one wishes to run qucumber on a CPU, add the flag “gpu = False” in the ComplexWaveFunction object instantiation. Uncomment the line above to run this tutorial on a GPU.

Now the hyperparameters of the training process can be specified.

  1. epochs: the total number of training cycles that will be performed (default = 100)

  2. pos_batch_size: the number of data points used in the positive phase of the gradient (default = 100)

  3. neg_batch_size: the number of data points used in the negative phase of the gradient (default = pos_batch_size)

  4. k: the number of contrastive divergence steps (default = 1)

  5. lr: the learning rate (default = 0.001)

    Note: For more information on the hyperparameters above, it is strongly encouraged that the user to read through the brief, but thorough theory document on RBMs. One does not have to specify these hyperparameters, as their default values will be used without the user overwriting them. It is recommended to keep with the default values until the user has a stronger grasp on what these hyperparameters mean. The quality and the computational efficiency of the training will highly depend on the choice of hyperparameters. As such, playing around with the hyperparameters is almost always necessary.

The two-qubit example in this tutorial should be extremely easy to train, regardless of the choice of hyperparameters. However, the hyperparameters below will be used.

[5]:

epochs = 100
pbs = 50  # pos_batch_size
nbs = 50  # neg_batch_size
lr = 0.1
k = 5

For evaluating the training in real time, the MetricEvaluator will be called to calculate the training evaluators every 10 epochs. The MetricEvaluator requires the following arguments.

  1. log_every: the frequency of the training evaluators being calculated is controlled by the log_every argument (e.g. log_every = 200 means that the MetricEvaluator will update the user every 200 epochs)
  2. A dictionary of functions you would like to reference to evaluate the training (arguments required for these functions are keyword arguments placed after the dictionary)

The following additional arguments are needed to calculate the fidelity and KL divergence in the training_statistics utility.

  • target_psi (the true wavefunction of the system)
  • space (the hilbert space of the system)

The training evaluators can be printed out via the verbose=True statement.

Although the fidelity and KL divergence are excellent training evaluators, they are not practical to calculate in most cases; the user may not have access to the target wavefunction of the system, nor may generating the hilbert space of the system be computationally feasible. However, evaluating the training in real time is extremely convenient.

Any custom function that the user would like to use to evaluate the training can be given to the MetricEvaluator, thus avoiding having to calculate fidelity and/or KL divergence. As an example, functions that calculate the the norm of each of the reconstructed wavefunction’s coefficients are presented. Any custom function given to MetricEvaluator must take the neural-network state (in this case, the ComplexWaveFunction object) and keyword arguments. Although the given example requires the hilbert space to be computed, the scope of the MetricEvaluator’s ability to be able to handle any function should still be evident.

[6]:

def alpha(nn_state, space, **kwargs):
    rbm_psi = nn_state.psi(space)
    normalization = nn_state.compute_normalization(space).sqrt_()
    alpha_ = cplx.norm(
        torch.tensor([rbm_psi[0][0], rbm_psi[1][0]], device=nn_state.device)
        / normalization
    )

    return alpha_


def beta(nn_state, space, **kwargs):
    rbm_psi = nn_state.psi(space)
    normalization = nn_state.compute_normalization(space).sqrt_()
    beta_ = cplx.norm(
        torch.tensor([rbm_psi[0][1], rbm_psi[1][1]], device=nn_state.device)
        / normalization
    )

    return beta_


def gamma(nn_state, space, **kwargs):
    rbm_psi = nn_state.psi(space)
    normalization = nn_state.compute_normalization(space).sqrt_()
    gamma_ = cplx.norm(
        torch.tensor([rbm_psi[0][2], rbm_psi[1][2]], device=nn_state.device)
        / normalization
    )

    return gamma_


def delta(nn_state, space, **kwargs):
    rbm_psi = nn_state.psi(space)
    normalization = nn_state.compute_normalization(space).sqrt_()
    delta_ = cplx.norm(
        torch.tensor([rbm_psi[0][3], rbm_psi[1][3]], device=nn_state.device)
        / normalization
    )

    return delta_

Now the hilbert space of the system must be generated for the fidelity and KL divergence and the dictionary of functions the user would like to compute every “log_every” epochs must be given to the MetricEvaluator.

[7]:

log_every = 2
space = nn_state.generate_hilbert_space(nv)

callbacks = [
    MetricEvaluator(
        log_every,
        {
            "Fidelity": ts.fidelity,
            "KL": ts.KL,
            "normα": alpha,
#             "normβ": beta,
#             "normγ": gamma,
#             "normδ": delta,
        },
        target_psi=true_psi,
        bases=bases,
        verbose=True,
        space=space,
    )
]

Now the training can begin. The ComplexWaveFunction object has a property called fit which takes care of this.

[8]:

nn_state.fit(
    train_samples,
    epochs=epochs,
    pos_batch_size=pbs,
    neg_batch_size=nbs,
    lr=lr,
    k=k,
    input_bases=train_bases,
    callbacks=callbacks,
)

Epoch: 2        Fidelity = 0.609290     KL = 0.251365   normα = 0.328561
Epoch: 4        Fidelity = 0.761520     KL = 0.130756   normα = 0.268571
Epoch: 6        Fidelity = 0.838254     KL = 0.082158   normα = 0.253614
Epoch: 8        Fidelity = 0.882321     KL = 0.059876   normα = 0.251210
Epoch: 10       Fidelity = 0.909942     KL = 0.046754   normα = 0.259010
Epoch: 12       Fidelity = 0.929755     KL = 0.036943   normα = 0.258238
Epoch: 14       Fidelity = 0.942398     KL = 0.030965   normα = 0.262524
Epoch: 16       Fidelity = 0.951771     KL = 0.027162   normα = 0.250808
Epoch: 18       Fidelity = 0.958536     KL = 0.023913   normα = 0.257332
Epoch: 20       Fidelity = 0.963766     KL = 0.021570   normα = 0.259561
Epoch: 22       Fidelity = 0.968224     KL = 0.019610   normα = 0.263528
Epoch: 24       Fidelity = 0.970991     KL = 0.018523   normα = 0.256601
Epoch: 26       Fidelity = 0.974414     KL = 0.017127   normα = 0.256168
Epoch: 28       Fidelity = 0.976543     KL = 0.016030   normα = 0.261707
Epoch: 30       Fidelity = 0.977891     KL = 0.015551   normα = 0.254371
Epoch: 32       Fidelity = 0.978768     KL = 0.015847   normα = 0.242762
Epoch: 34       Fidelity = 0.981126     KL = 0.013974   normα = 0.259100
Epoch: 36       Fidelity = 0.981330     KL = 0.013704   normα = 0.262152
Epoch: 38       Fidelity = 0.981989     KL = 0.013495   normα = 0.256111
Epoch: 40       Fidelity = 0.983230     KL = 0.012711   normα = 0.269000
Epoch: 42       Fidelity = 0.984230     KL = 0.012301   normα = 0.273091
Epoch: 44       Fidelity = 0.984190     KL = 0.012178   normα = 0.260481
Epoch: 46       Fidelity = 0.985494     KL = 0.011501   normα = 0.269168
Epoch: 48       Fidelity = 0.985192     KL = 0.011518   normα = 0.269217
Epoch: 50       Fidelity = 0.986754     KL = 0.010896   normα = 0.264035
Epoch: 52       Fidelity = 0.987266     KL = 0.011288   normα = 0.263792
Epoch: 54       Fidelity = 0.987998     KL = 0.010323   normα = 0.268859
Epoch: 56       Fidelity = 0.987993     KL = 0.009957   normα = 0.267215
Epoch: 58       Fidelity = 0.988191     KL = 0.009873   normα = 0.273412
Epoch: 60       Fidelity = 0.988129     KL = 0.009665   normα = 0.264751
Epoch: 62       Fidelity = 0.986891     KL = 0.010557   normα = 0.254349
Epoch: 64       Fidelity = 0.988134     KL = 0.009504   normα = 0.264387
Epoch: 66       Fidelity = 0.987419     KL = 0.009870   normα = 0.263105
Epoch: 68       Fidelity = 0.988299     KL = 0.009280   normα = 0.264269
Epoch: 70       Fidelity = 0.989128     KL = 0.008897   normα = 0.267263
Epoch: 72       Fidelity = 0.989572     KL = 0.008808   normα = 0.268239
Epoch: 74       Fidelity = 0.988996     KL = 0.008901   normα = 0.256966
Epoch: 76       Fidelity = 0.988131     KL = 0.009278   normα = 0.261540
Epoch: 78       Fidelity = 0.989458     KL = 0.008405   normα = 0.263894
Epoch: 80       Fidelity = 0.988967     KL = 0.008628   normα = 0.261319
Epoch: 82       Fidelity = 0.989337     KL = 0.008332   normα = 0.271008
Epoch: 84       Fidelity = 0.989170     KL = 0.008351   normα = 0.270172
Epoch: 86       Fidelity = 0.989256     KL = 0.008291   normα = 0.273329
Epoch: 88       Fidelity = 0.989592     KL = 0.008019   normα = 0.269137
Epoch: 90       Fidelity = 0.989677     KL = 0.007917   normα = 0.266120
Epoch: 92       Fidelity = 0.989260     KL = 0.008174   normα = 0.261290
Epoch: 94       Fidelity = 0.990006     KL = 0.007627   normα = 0.266389
Epoch: 96       Fidelity = 0.989957     KL = 0.007610   normα = 0.270035
Epoch: 98       Fidelity = 0.990623     KL = 0.007506   normα = 0.278505
Epoch: 100      Fidelity = 0.990754     KL = 0.007096   normα = 0.266719

All of these training evaluators can be accessed after the training has completed, as well. The code below shows this, along with plots of each training evaluator versus the training cycle number (epoch).

[9]:

fidelities = callbacks[0].Fidelity
KLs = callbacks[0].KL
coeffs = callbacks[0].normα
# Please note that the key given to the *MetricEvaluator* must be what comes after callbacks[0].
epoch = np.arange(log_every, epochs + 1, log_every)

[10]:

# Some parameters to make the plots look nice
params = {'text.usetex': True,
            'font.family': 'serif',
            'legend.fontsize': 14,
            'figure.figsize': (10, 3),
            'axes.labelsize': 16,
            'xtick.labelsize':14,
            'ytick.labelsize':14,
            'lines.linewidth':2,
            'lines.markeredgewidth': 0.8,
            'lines.markersize': 5,
            'lines.marker': "o",
            "patch.edgecolor": "black"
         }
plt.rcParams.update(params)
plt.style.use('seaborn-deep')

[11]:

fig, axs = plt.subplots(nrows=1, ncols=3, figsize=(14, 3))
ax = axs[0]
ax.plot(epoch, fidelities, "o", color = "C0", markeredgecolor="black")
ax.set_ylabel(r'Fidelity')
ax.set_xlabel(r'Epoch')

ax = axs[1]
ax.plot(epoch, KLs, "o", color = "C1", markeredgecolor="black")
ax.set_ylabel(r'KL Divergence')
ax.set_xlabel(r'Epoch')

ax = axs[2]
ax.plot(epoch, coeffs, "o", color = "C2", markeredgecolor="black")
ax.set_ylabel(r'$\vert\alpha\vert$')
ax.set_xlabel(r'Epoch')

plt.tight_layout()
plt.savefig("complex_fid_KL.pdf")
plt.show()
_images/_examples_Tutorial2_TrainComplexWaveFunction_tutorial_qubits_19_0.png

It should be noted that one could have just ran nn_state.fit(train_samples) and just used the default hyperparameters and no training evaluators.

At the end of the training process, the network parameters (the weights, visible biases and hidden biases) are stored in the ComplexWaveFunction object. One can save them to a pickle file, which will be called saved_params.pt, with the following command.

[12]:

nn_state.save("saved_params.pt")

This saves the weights, visible biases and hidden biases as torch tensors with the following keys: “weights”, “visible_bias”, “hidden_bias”.

This is a static, non-editable tutorial.

We recommend you install QuCumber if you want to run the examples locally. You can then get an archive file containing the examples from the relevant release here. Alternatively, you can launch an interactive online version, though it may be a bit slow: Binder badge

Sampling and calculating observables

Generate new samples

Firstly, to generate meaningful data, an RBM needs to be trained. Please refer to the tutorials 1 and 2 on training an RBM if how to train an RBM using qucumber is unclear. An RBM with a positive-real wavefunction describing a transverse-field Ising model (TFIM) with 10 sites has already been trained in the first tutorial, with the parameters of the machine saved here as saved_params.pt. The autoload function can be employed here to instantiate the corresponding PositiveWaveFunction object from the saved RBM parameters.

[1]:

import numpy as np
import matplotlib.pyplot as plt

from qucumber.nn_states import PositiveWaveFunction

from qucumber.observables import ObservableBase

import quantum_ising_chain
from quantum_ising_chain import TFIMChainEnergy

nn_state = PositiveWaveFunction.autoload("saved_params.pt")

A PositiveWaveFunction object has a property called sample that takes in the following arguments.

  1. k: the number of Gibbs steps to perform to generate the new samples
  2. num_samples: the number of new data points to be generated
[2]:

new_samples = nn_state.sample(k=100, num_samples=10000)
print(new_samples)

tensor([[1., 1., 1.,  ..., 1., 0., 0.],
        [1., 1., 1.,  ..., 1., 0., 0.],
        [0., 0., 0.,  ..., 0., 1., 1.],
        ...,
        [1., 1., 1.,  ..., 1., 1., 1.],
        [0., 0., 1.,  ..., 0., 1., 1.],
        [0., 0., 0.,  ..., 1., 1., 1.]], dtype=torch.float64)

With the newly generated samples, the user can now easliy calculate observables that do not require any details associated with the RBM. A great example of this is the magnetization. To calculate the magnetization, the newly-generated samples must be converted to \pm 1 from 1 and 0, respectively. The function below does the trick.

[3]:

def to_pm1(samples):
    return samples.mul(2.).sub(1.)

Now, the magnetization is calculated as follows.

[4]:

def Magnetization(samples):
    return to_pm1(samples).mean(1).abs().mean()


magnetization = Magnetization(new_samples).item()

print("Magnetization = %.5f" % magnetization)

Magnetization = 0.54968

The exact value for the magnetization is 0.5610.

The magnetization and the newly-generated samples can also be saved to a pickle file along with the RBM parameters in the PositiveWaveFunction object.

[5]:

nn_state.save(
    "saved_params_and_new_data.pt",
    metadata={"samples": new_samples, "magnetization": magnetization},
)

The metadata argument in the save function takes in a dictionary of data that you would like to save on top of the RBM parameters.

Calculate an observable using the Observable module

Custom observable

Qucumber has a built-in module called Observable which makes it easy for the user to compute any arbitrary observable from the RBM. To see the the Observable module in action, an example observable called PIQuIL, which inherits properties from the Observable module, is shown below.

The PIQuIL observable takes an \sigma^z measurement at a site and multiplies it by the measurement two sites from it. There is also a parameter, P, that determines the strength of each of these interactions. For example, for the dataset (-1,1,1,-1), (1,1,1,1) and (1,1,-1,1) with P = 2, the PIQuIL for each data point would be \left( 2(-1\times1) + 2(1\times-1) = -4 \right), \left( 2(1\times1) + 2(1\times1) = 4 \right) and \left( 2(1\times-1) + 2(1\times1) = 0 \right), respectively.

[6]:

class PIQuIL(ObservableBase):
    def __init__(self, P):
        super(PIQuIL, self).__init__()
        self.P = P

    # Required : function that calculates the PIQuIL. Must be named "apply"
    def apply(self, nn_state, samples):
        to_pm1(samples)
        interaction_ = 0
        for i in range(samples.shape[-1]):
            if (i + 3) > samples.shape[-1]:
                continue
            else:
                interaction_ += self.P * samples[:, i] * samples[:, i + 2]

        return interaction_


P = 0.05
piquil = PIQuIL(P)

The apply function is contained in the Observable module, but is overwritten here. The apply function in Observable will compute the observable itself and must take in the RBM (nn_state) and a batch of samples as arguments. Thus, any new class inheriting from Observables that the user would like to define must contain a function called apply that calculates this new observable.

Although the PIQuIL observable could technically be computed without the use of the Observable module since it does not ever use the RBM (nn_state), it is still nonetheless a constructive example.

The real power in the Observable module is in the ability for the user to easily compute statistics of the observable from the generated sample. Since we have already generated new samples of data, the PIQuIL observable’s mean, standard error and variance on the new data can be calculated with the statistics_from_samples function in the Observable module. The user must simply give the RBM and the samples as arguments.

[7]:

piquil_stats1 = piquil.statistics_from_samples(nn_state, new_samples)

The statistics_from_samples function returns a dictionary containing the mean, standard error and the variance with the keys “mean”, “std_error” and “variance”, respectively.

[8]:

print(
    "Mean PIQuIL: %.4f" % piquil_stats1["mean"], "+/- %.4f" % piquil_stats1["std_error"]
)
print("Variance: %.4f" % piquil_stats1["variance"])

Mean PIQuIL: 0.1419 +/- 0.0014
Variance: 0.0188

However, if the user did not have samples generated already, that is no problem. The statistics function in the Observable module will generate new samples internally and compute the mean, standard error and variance on those samples. Since the samples are not an argument in the statistics function, the user must now give the following additional arguments to the statistics function to generate the new samples.

  • num_samples: the number of samples to generate internally
  • num_chains: the number of Markov chains to run in parallel (default = 0)
  • burn_in: the number of Gibbs steps to perform before recording any samples (default = 1000)
  • steps: the number of Gibbs steps to perform between each sample (default = 1)

The statistics function will also return a dictionary containing the mean, standard error and the variance with the keys “mean”, “std_error” and “variance”, respectively.

[9]:

num_samples = 10000
burn_in = 100
steps = 100

piquil_stats2 = piquil.statistics(nn_state, num_samples, burn_in=burn_in, steps=steps)
print(
    "Mean PIQuIL: %.4f" % piquil_stats2["mean"], "+/- %.4f" % piquil_stats2["std_error"]
)
print("Variance: %.4f" % piquil_stats2["variance"])

Mean PIQuIL: 0.1409 +/- 0.0014
Variance: 0.0186

TFIM Energy

Some observables cannot be computed directly from samples, but instead depend on the RBM as previously mentioned. For example, the magnetization of the TFIM simply depends on the samples the user gives as input. Whereas the TFIM energy is much more complicated. An example for the computation of the energy is provided in the python file quantum_ising_chain.py, which takes advantage of qucumber’s Observable module.

quantum_ising_chain.py comprises of a class that computes the energy of a TFIM (TFIMChainEnergy) that inherits properties from the Observable module. To instantiate a TFIMChainEnergy object, the \frac{h}{J} value must be specified. The trained RBM parameters are from the first tutorial, where the example data was from the TFIM with 10 sites at its critical point (\frac{h}{J}=1).

[10]:

h = 1

tfim_energy = TFIMChainEnergy(h)

To go ahead and calculate the mean energy and its standard error from the previously generated samples from this tutorial (new_samples), the statistics_from_samples function in the Observable module is called upon.

[11]:

energy_stats = tfim_energy.statistics_from_samples(nn_state, new_samples)
print("Mean: %.4f" % energy_stats["mean"], "+/- %.4f" % energy_stats["std_error"])
print("Variance: %.4f" % energy_stats["variance"])

Mean: -1.2362 +/- 0.0005
Variance: 0.0022

The exact value for the energy is -1.2381.

To illustrate how quickly the energy converges as a function of the sampling step (i.e. the number of Gibbs steps to perform to generate a new batch of samples), steps, the Convergence function in quantum_ising_chain.py will do the trick. Convergence creates a batch of random samples initially, which is then used to generate a new batch of samples from the RBM. The TFIM energy will be calculated at every Gibbs step. Please note that the samples generated previously (new_samples) are not used here; different samples are generated.

[12]:

steps = 200
num_samples = 10000

dict_observables = quantum_ising_chain.Convergence(
    nn_state, tfim_energy, num_samples, steps
)

energy = dict_observables["energies"]
err_energy = dict_observables["error"]

step = np.arange(steps + 1)

E0 = -1.2381

ax = plt.axes()
ax.plot(step, abs((energy - E0) / E0) * 100, color="red")
ax.set_xlim(0, steps)
ax.set_ylim(0, 0.6)
ax.set_xlabel("Gibbs Step")
ax.set_ylabel("% Error in Energy")

[12]:

Text(0,0.5,'% Error in Energy')
_images/_examples_Tutorial3_DataGeneration_CalculateObservables_tutorial_sampling_observables_24_1.png

One can see a brief transient period in the magnetization observable, before the state of the machine “warms up” to equilibrium. After that, the values fluctuate around the calculated mean.

Adding observables

One may also add / subtract observables with the new observable also retaining the same properties in the Observables module. For instance, a new observable can be defined by adding the TFIM energy observable multiplied by an arbitrary constant to the PIQuIL observable.

[13]:

new_obs = 0.01 * tfim_energy + piquil

The same statistics of this new observable can also be calculated.

[14]:

new_obs_stats = new_obs.statistics_from_samples(nn_state, new_samples)
print("Mean: %.4f" % new_obs_stats["mean"], "+/- %.4f" % new_obs_stats["std_error"])
print("Variance: %.4f" % new_obs_stats["variance"])

Mean: 0.1295 +/- 0.0014
Variance: 0.0188

Template for your custom observable

Here is a generic template for you to try using the Observable module yourself.

[15]:

import torch
from qucumber.observables import ObservableBase


class YourObservable(ObservableBase):
    def __init__(self, your_constants):
        super(YourObservable, self).__init__()
        self.your_constants = your_constants

    def apply(self, nn_state, samples):
        # arguments of "apply" must be in this order

        # calculate your observable for each data point
        obs = torch.tensor([42] * len(samples))

        # make sure the observables are on the same device and have the
        # same dtype as the samples
        obs = obs.to(samples)

        # return a torch tensor containing the observable values
        return obs

This is a static, non-editable tutorial.

We recommend you install QuCumber if you want to run the examples locally. You can then get an archive file containing the examples from the relevant release here. Alternatively, you can launch an interactive online version, though it may be a bit slow: Binder badge

Training while monitoring observables

As seen in the first tutorial that went through reconstructing the wavefunction describing the TFIM with 10 sites at its critical point, the user can evaluate the training in real time with the MetricEvaluator and custom functions. What is most likely more impactful in many cases is to calculate an observable, like the energy, during the training process. This is slightly more computationally involved than using the MetricEvaluator to evaluate functions because observables require that samples be drawn from the RBM.

Luckily, qucumber also has a module very similar to the MetricEvaluator, but for observables. This is called the ObservableEvaluator. The following implements the ObservableEvaluator to calculate the energy during the training on the TFIM data in the first tutorial. We will use the same hyperparameters as before.

It is assumed that the user has worked through tutorial 3 beforehand. Recall that quantum_ising_chain.py contains the TFIMChainEnergy class that inherits from the Observable module. The exact ground-state energy is -1.2381.

[1]:

import os.path

import numpy as np
import matplotlib.pyplot as plt

from qucumber.nn_states import PositiveWaveFunction
from qucumber.callbacks import ObservableEvaluator

import qucumber.utils.data as data

from quantum_ising_chain import TFIMChainEnergy

[2]:

train_data = data.load_data(
    os.path.join("..", "Tutorial1_TrainPosRealWaveFunction", "tfim1d_data.txt")
)[0]

nv = train_data.shape[-1]
nh = nv

nn_state = PositiveWaveFunction(num_visible=nv, num_hidden=nh)

epochs = 1000
pbs = 100  # pos_batch_size
nbs = 200  # neg_batch_size
lr = 0.01
k = 10

log_every = 100

h = 1
num_samples = 10000
burn_in = 100
steps = 100

tfim_energy = TFIMChainEnergy(h)

Now, the ObservableEvaluator can be called. The ObservableEvaluator requires the following arguments.

  1. log_every: the frequency of the training evaluators being calculated is controlled by the log_every argument (e.g. log_every = 200 means that the MetricEvaluator will update the user every 200 epochs)
  2. A list of Observable objects you would like to reference to evaluate the training (arguments required for generating samples to calculate the observables are keyword arguments placed after the list)

The following additional arguments are needed to calculate the statistics on the generated samples during training (these are the arguments of the statistics function in the Observable module, minus the nn_state argument; this gets passed in as an argument to fit).

  • num_samples: the number of samples to generate internally
  • num_chains: the number of Markov chains to run in parallel (default = 0)
  • burn_in: the number of Gibbs steps to perform before recording any samples (default = 1000)
  • steps: the number of Gibbs steps to perform between each sample (default = 1)

The training evaluators can be printed out via the verbose=True statement.

[3]:

callbacks = [
    ObservableEvaluator(
        log_every,
        [tfim_energy],
        verbose=True,
        num_samples=num_samples,
        burn_in=burn_in,
        steps=steps,
    )
]

nn_state.fit(
    train_data,
    epochs=epochs,
    pos_batch_size=pbs,
    neg_batch_size=nbs,
    lr=lr,
    k=k,
    callbacks=callbacks,
)

Epoch: 100
  TFIMChainEnergy:
    mean: -1.197008     variance: 0.022882      std_error: 0.001513
Epoch: 200
  TFIMChainEnergy:
    mean: -1.216405     variance: 0.011845      std_error: 0.001088
Epoch: 300
  TFIMChainEnergy:
    mean: -1.224917     variance: 0.008271      std_error: 0.000909
Epoch: 400
  TFIMChainEnergy:
    mean: -1.228988     variance: 0.005977      std_error: 0.000773
Epoch: 500
  TFIMChainEnergy:
    mean: -1.230748     variance: 0.004908      std_error: 0.000701
Epoch: 600
  TFIMChainEnergy:
    mean: -1.232201     variance: 0.003850      std_error: 0.000620
Epoch: 700
  TFIMChainEnergy:
    mean: -1.233295     variance: 0.003404      std_error: 0.000583
Epoch: 800
  TFIMChainEnergy:
    mean: -1.233561     variance: 0.002842      std_error: 0.000533
Epoch: 900
  TFIMChainEnergy:
    mean: -1.235249     variance: 0.002480      std_error: 0.000498
Epoch: 1000
  TFIMChainEnergy:
    mean: -1.234220     variance: 0.002232      std_error: 0.000472

The callbacks list returns a list of dictionaries. The mean, standard error and the variance at each epoch can be accessed as follows.

[4]:

energies = callbacks[0].TFIMChainEnergy.mean
errors = callbacks[0].TFIMChainEnergy.std_error
variance = callbacks[0].TFIMChainEnergy.variance
# Please note that the name of the observable class that the user makes must be what comes after callbacks[0].

A plot of the energy as a function of the training cycle is presented below.

[5]:

epoch = np.arange(log_every, epochs + 1, log_every)

E0 = -1.2381

ax = plt.axes()
ax.plot(epoch, energies, color="red")
ax.set_xlim(log_every, epochs)
ax.axhline(E0, color="black")
ax.fill_between(epoch, energies - errors, energies + errors, alpha=0.2, color="black")
ax.set_xlabel("Epoch")
ax.set_ylabel("Energy")
ax.grid()
_images/_examples_Tutorial4_MonitoringObservables_tutorial_monitor_observables_8_0.png

RBM

class qucumber.rbm.BinaryRBM(num_visible, num_hidden, zero_weights=False, gpu=True)[source]

Bases: torch.nn.modules.module.Module

effective_energy(v)[source]

The effective energies of the given visible states.

\mathcal{E}(\bm{v}) &= -\sum_{j}b_j v_j - \sum_{i}\log \left\lbrack 1 + \exp\left(c_{i} + \sum_{j} W_{ij} v_j\right) \right\rbrack

Parameters:v (torch.Tensor) – The visible states.
Returns:The effective energies of the given visible states.
Return type:torch.Tensor
effective_energy_gradient(v)[source]

The gradients of the effective energies for the given visible states.

Parameters:v (torch.Tensor) – The visible states.
Returns:1d vector containing the gradients for all parameters (computed on the given visible states v).
Return type:torch.Tensor
gibbs_steps(k, initial_state, overwrite=False)[source]

Performs k steps of Block Gibbs sampling. One step consists of sampling the hidden state \bm{h} from the conditional distribution p(\bm{h}\:|\:\bm{v}), and sampling the visible state \bm{v} from the conditional distribution p(\bm{v}\:|\:\bm{h}).

Parameters:
  • k (int) – Number of Block Gibbs steps.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided.
initialize_parameters(zero_weights=False)[source]

Randomize the parameters of the RBM

partition(space)[source]

Compute the partition function of the RBM.

Parameters:space (torch.Tensor) – A rank 2 tensor of the visible space.
Returns:The value of the partition function evaluated at the current state of the RBM.
Return type:torch.Tensor
prob_h_given_v(v, out=None)[source]

Given a visible unit configuration, compute the probability vector of the hidden units being on.

Parameters:
Returns:

The probability of hidden units being active given the visible state.
Return type:

torch.Tensor
prob_v_given_h(h, out=None)[source]

Given a hidden unit configuration, compute the probability vector of the visible units being on.

Parameters:
Returns:

The probability of visible units being active given the hidden state.
Return type:

torch.Tensor
sample_h_given_v(v, out=None)[source]

Sample/generate a hidden state given a visible state.

Parameters:
Returns:

Tuple containing prob_h_given_v(v) and the sampled hidden state.
Return type:

tuple(torch.Tensor, torch.Tensor)
sample_v_given_h(h, out=None)[source]

Sample/generate a visible state given a hidden state.

Parameters:
Returns:

Tuple containing prob_v_given_h(h) and the sampled visible state.
Return type:

tuple(torch.Tensor, torch.Tensor)

Quantum States

Positive WaveFunction

class qucumber.nn_states.PositiveWaveFunction(num_visible, num_hidden=None, gpu=True)[source]

Bases: qucumber.nn_states.WaveFunctionBase

Class capable of learning wavefunctions with no phase.

Parameters:
  • num_visible (int) – The number of visible units, ie. the size of the system being learned.
  • num_hidden (int) – The number of hidden units in the internal RBM. Defaults to the number of visible units.
  • gpu (bool) – Whether to perform computations on the default gpu.
amplitude(v)[source]

Compute the (unnormalized) amplitude of a given vector/matrix of visible states.

\text{amplitude}(\bm{\sigma})=|\psi_{\bm{\lambda}}(\bm{\sigma})|= e^{-\mathcal{E}_{\bm{\lambda}}(\bm{\sigma})/2}

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Matrix/vector containing the amplitudes of v
Return type:torch.Tensor
static autoload(location, gpu=False)[source]

Initializes a WaveFunction from the parameters in the given location.

Parameters:
  • location (str or file) – The location to load the model parameters from.
  • gpu (bool) – Whether the returned model should be on the GPU.
Returns:

A new WaveFunction initialized from the given parameters. The returned WaveFunction will be of whichever type this function was called on.
compute_batch_gradients(k, samples_batch, neg_batch)[source]

Compute the gradients of a batch of the training data (samples_batch).

Parameters:
  • k (int) – Number of contrastive divergence steps in training.
  • samples_batch (torch.Tensor) – Batch of the input samples.
  • neg_batch (torch.Tensor) – Batch of the input samples for computing the negative phase.
Returns:

List containing the gradients of the parameters.
Return type:

list
compute_normalization(space)[source]

Compute the normalization constant of the wavefunction.

Z_{\bm{\lambda}}=\sqrt{\sum_{\bm{\sigma}}|\psi_{\bm{\lambda}}|^2}= \sqrt{\sum_{\bm{\sigma}} p_{\bm{\lambda}}(\bm{\sigma})}

Parameters:space (torch.Tensor) – A rank 2 tensor of the entire visible space.
device

The device that the model is on.

fit(data, epochs=100, pos_batch_size=100, neg_batch_size=None, k=1, lr=0.001, progbar=False, starting_epoch=1, time=False, callbacks=None, optimizer=<class 'torch.optim.sgd.SGD'>, **kwargs)[source]

Train the WaveFunction.

Parameters:
  • data (np.array) – The training samples
  • epochs (int) – The number of full training passes through the dataset. Technically, this specifies the index of the last training epoch, which is relevant if starting_epoch is being set.
  • pos_batch_size (int) – The size of batches for the positive phase taken from the data.
  • neg_batch_size (int) – The size of batches for the negative phase taken from the data. Defaults to pos_batch_size.
  • k (int) – The number of contrastive divergence steps.
  • lr (float) – Learning rate
  • progbar (bool or str) – Whether or not to display a progress bar. If “notebook” is passed, will use a Jupyter notebook compatible progress bar.
  • starting_epoch (int) – The epoch to start from. Useful if continuing training from a previous state.
  • callbacks (list[qucumber.callbacks.CallbackBase]) – Callbacks to run while training.
  • optimizer (torch.optim.Optimizer) – The constructor of a torch optimizer.
  • kwargs – Keyword arguments to pass to the optimizer
generate_hilbert_space(size=None, device=None)[source]

Generates Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space. Defaults to the number of visible units.
  • device – The device to create the Hilbert space matrix on. Defaults to the device this model is on.
Returns:

A tensor with all the basis states of the Hilbert space.
Return type:

torch.Tensor
gradient(v)[source]

Compute the gradient of the effective energy for a batch of states.

\nabla_{\bm{\lambda}}\mathcal{E}_{\bm{\lambda}}(\bm{\sigma})

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:A single tensor containing all of the parameter gradients.
Return type:torch.Tensor
load(location)[source]

Loads the WaveFunction parameters from the given location ignoring any metadata stored in the file. Overwrites the WaveFunction’s parameters.

Note

The WaveFunction object on which this function is called must have the same parameter shapes as the one who’s parameters are being loaded.

Parameters:location (str or file) – The location to load the WaveFunction parameters from.
max_size

Maximum size of the Hilbert space for full enumeration

networks

A list of the names of the internal RBMs.

phase(v)[source]

Compute the phase of a given vector/matrix of visible states.

In the case of a PositiveWaveFunction, the phase is just zero.

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Matrix/vector containing the phases of v
Return type:torch.Tensor
probability(v, Z)[source]

Evaluates the probability of the given vector(s) of visible states.

Parameters:
Returns:

The probability of the given vector(s) of visible units.
Return type:

torch.Tensor
psi(v)[source]

Compute the (unnormalized) wavefunction of a given vector/matrix of visible states.

\psi_{\bm{\lambda}}(\bm{\sigma}) = e^{-\mathcal{E}_{\bm{\lambda}}(\bm{\sigma})/2}

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Complex object containing the value of the wavefunction for each visible state
Return type:torch.Tensor
rbm_am

The RBM to be used to learn the wavefunction amplitude.

reinitialize_parameters()[source]

Randomize the parameters of the internal RBMs.

sample(k, num_samples=1, initial_state=None, overwrite=False)[source]

Performs k steps of Block Gibbs sampling. One step consists of sampling the hidden state \bm{h} from the conditional distribution p_{\bm{\lambda}}(\bm{h}\:|\:\bm{v}), and sampling the visible state \bm{v} from the conditional distribution p_{\bm{\lambda}}(\bm{v}\:|\:\bm{h}).

Parameters:
  • k (int) – Number of Block Gibbs steps.
  • num_samples (int) – The number of samples to generate.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided.
save(location, metadata=None)[source]

Saves the WaveFunction parameters to the given location along with any given metadata.

Parameters:
  • location (str or file) – The location to save the data.
  • metadata (dict) – Any extra metadata to store alongside the WaveFunction parameters.
stop_training

If True, will not train.

If this property is set to True during the training cycle, training will terminate once the current batch or epoch ends (depending on when stop_training was set).

subspace_vector(num, size=None, device=None)[source]

Generates a single vector from the Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space.
  • num (int) – The specific vector to return from the Hilbert space. Since the Hilbert space can be represented by the set of binary strings of length size, num is equivalent to the decimal representation of the returned vector.
  • device – The device to create the vector on. Defaults to the device this model is on.
Returns:

A state from the Hilbert space.
Return type:

torch.Tensor

Complex WaveFunction

class qucumber.nn_states.ComplexWaveFunction(num_visible, num_hidden=None, unitary_dict=None, gpu=True)[source]

Bases: qucumber.nn_states.WaveFunctionBase

Class capable of learning wavefunctions with a non-zero phase.

Parameters:
  • num_visible (int) – The number of visible units, ie. the size of the system being learned.
  • num_hidden (int) – The number of hidden units in both internal RBMs. Defaults to the number of visible units.
  • unitary_dict (dict[str, torch.Tensor]) – A dictionary mapping unitary names to their matrix representations.
  • gpu (bool) – Whether to perform computations on the default gpu.
amplitude(v)[source]

Compute the (unnormalized) amplitude of a given vector/matrix of visible states.

\text{amplitude}(\bm{\sigma})=|\psi_{\bm{\lambda\mu}}(\bm{\sigma})|= e^{-\mathcal{E}_{\bm{\lambda}}(\bm{\sigma})/2}

Parameters:v (torch.Tensor) – visible states \bm{\sigma}.
Returns:Vector containing the amplitudes of the given states.
Return type:torch.Tensor
static autoload(location, gpu=False)[source]

Initializes a WaveFunction from the parameters in the given location.

Parameters:
  • location (str or file) – The location to load the model parameters from.
  • gpu (bool) – Whether the returned model should be on the GPU.
Returns:

A new WaveFunction initialized from the given parameters. The returned WaveFunction will be of whichever type this function was called on.
compute_batch_gradients(k, samples_batch, neg_batch, bases_batch=None)[source]

Compute the gradients of a batch of the training data (samples_batch).

If measurements are taken in bases other than the reference basis, a list of bases (bases_batch) must also be provided.

Parameters:
  • k (int) – Number of contrastive divergence steps in training.
  • samples_batch (torch.Tensor) – Batch of the input samples.
  • neg_batch (torch.Tensor) – Batch of the input samples for computing the negative phase.
  • bases_batch (np.array) – Batch of the input bases corresponding to the samples in samples_batch.
Returns:

List containing the gradients of the parameters.
Return type:

list
compute_normalization(space)[source]

Compute the normalization constant of the wavefunction.

Z_{\bm{\lambda}}= \sqrt{\sum_{\bm{\sigma}}|\psi_{\bm{\lambda\mu}}|^2}= \sqrt{\sum_{\bm{\sigma}} p_{\bm{\lambda}}(\bm{\sigma})}

Parameters:space (torch.Tensor) – A rank 2 tensor of the entire visible space.
device

The device that the model is on.

fit(data, epochs=100, pos_batch_size=100, neg_batch_size=None, k=1, lr=0.001, input_bases=None, progbar=False, starting_epoch=1, time=False, callbacks=None, optimizer=<class 'torch.optim.sgd.SGD'>, **kwargs)[source]

Train the WaveFunction.

Parameters:
  • data (np.array) – The training samples
  • epochs (int) – The number of full training passes through the dataset. Technically, this specifies the index of the last training epoch, which is relevant if starting_epoch is being set.
  • pos_batch_size (int) – The size of batches for the positive phase taken from the data.
  • neg_batch_size (int) – The size of batches for the negative phase taken from the data. Defaults to pos_batch_size.
  • k (int) – The number of contrastive divergence steps.
  • lr (float) – Learning rate
  • input_bases (np.array) – The measurement bases for each sample. Must be provided if training a ComplexWaveFunction.
  • progbar (bool or str) – Whether or not to display a progress bar. If “notebook” is passed, will use a Jupyter notebook compatible progress bar.
  • starting_epoch (int) – The epoch to start from. Useful if continuing training from a previous state.
  • callbacks (list[qucumber.callbacks.CallbackBase]) – Callbacks to run while training.
  • optimizer (torch.optim.Optimizer) – The constructor of a torch optimizer.
  • kwargs – Keyword arguments to pass to the optimizer
generate_hilbert_space(size=None, device=None)[source]

Generates Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space. Defaults to the number of visible units.
  • device – The device to create the Hilbert space matrix on. Defaults to the device this model is on.
Returns:

A tensor with all the basis states of the Hilbert space.
Return type:

torch.Tensor
gradient(basis, sample)[source]

Compute the gradient of a sample, measured in different bases.

Parameters:
  • basis (np.array) – A set of bases.
  • sample (np.array) – A sample to compute the gradient of.
Returns:

A list of 2 tensors containing the parameters of each of the internal RBMs.
Return type:

list[torch.Tensor]
load(location)[source]

Loads the WaveFunction parameters from the given location ignoring any metadata stored in the file. Overwrites the WaveFunction’s parameters.

Note

The WaveFunction object on which this function is called must have the same parameter shapes as the one who’s parameters are being loaded.

Parameters:location (str or file) – The location to load the WaveFunction parameters from.
max_size

Maximum size of the Hilbert space for full enumeration

networks

A list of the names of the internal RBMs.

phase(v)[source]

Compute the phase of a given vector/matrix of visible states.

\text{phase}(\bm{\sigma})=-\mathcal{E}_{\bm{\mu}}(\bm{\sigma})/2

Parameters:v (torch.Tensor) – visible states \bm{\sigma}.
Returns:Vector containing the phases of the given states.
Return type:torch.Tensor
probability(v, Z)[source]

Evaluates the probability of the given vector(s) of visible states.

Parameters:
Returns:

The probability of the given vector(s) of visible units.
Return type:

torch.Tensor
psi(v)[source]

Compute the (unnormalized) wavefunction of a given vector/matrix of visible states.

\psi_{\bm{\lambda\mu}}(\bm{\sigma}) = e^{-[\mathcal{E}_{\bm{\lambda}}(\bm{\sigma}) + i\mathcal{E}_{\bm{\mu}}(\bm{\sigma})]/2}

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Complex object containing the value of the wavefunction for each visible state
Return type:torch.Tensor
rbm_am

The RBM to be used to learn the wavefunction amplitude.

rbm_ph

RBM used to learn the wavefunction phase.

reinitialize_parameters()[source]

Randomize the parameters of the internal RBMs.

sample(k, num_samples=1, initial_state=None, overwrite=False)[source]

Performs k steps of Block Gibbs sampling. One step consists of sampling the hidden state \bm{h} from the conditional distribution p_{\bm{\lambda}}(\bm{h}\:|\:\bm{v}), and sampling the visible state \bm{v} from the conditional distribution p_{\bm{\lambda}}(\bm{v}\:|\:\bm{h}).

Parameters:
  • k (int) – Number of Block Gibbs steps.
  • num_samples (int) – The number of samples to generate.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided.
save(location, metadata=None)[source]

Saves the WaveFunction parameters to the given location along with any given metadata.

Parameters:
  • location (str or file) – The location to save the data.
  • metadata (dict) – Any extra metadata to store alongside the WaveFunction parameters.
stop_training

If True, will not train.

If this property is set to True during the training cycle, training will terminate once the current batch or epoch ends (depending on when stop_training was set).

subspace_vector(num, size=None, device=None)[source]

Generates a single vector from the Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space.
  • num (int) – The specific vector to return from the Hilbert space. Since the Hilbert space can be represented by the set of binary strings of length size, num is equivalent to the decimal representation of the returned vector.
  • device – The device to create the vector on. Defaults to the device this model is on.
Returns:

A state from the Hilbert space.
Return type:

torch.Tensor

Abstract WaveFunction

Note

This is an Abstract Base Class, it is not meant to be used directly. The following API reference is mostly for developers.

class qucumber.nn_states.WaveFunctionBase[source]

Bases: abc.ABC

Abstract Base Class for WaveFunctions.

amplitude(v)[source]

Compute the (unnormalized) amplitude of a given vector/matrix of visible states.

\text{amplitude}(\bm{\sigma})=|\psi(\bm{\sigma})|

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Matrix/vector containing the amplitudes of v
Return type:torch.Tensor
static autoload(location, gpu=False)[source]

Initializes a WaveFunction from the parameters in the given location.

Parameters:
  • location (str or file) – The location to load the model parameters from.
  • gpu (bool) – Whether the returned model should be on the GPU.
Returns:

A new WaveFunction initialized from the given parameters. The returned WaveFunction will be of whichever type this function was called on.
compute_batch_gradients(k, samples_batch, neg_batch, bases_batch=None)[source]

Compute the gradients of a batch of the training data (samples_batch).

If measurements are taken in bases other than the reference basis, a list of bases (bases_batch) must also be provided.

Parameters:
  • k (int) – Number of contrastive divergence steps in training.
  • samples_batch (torch.Tensor) – Batch of the input samples.
  • neg_batch (torch.Tensor) – Batch of the input samples for computing the negative phase.
  • bases_batch (np.array) – Batch of the input bases corresponding to the samples in samples_batch.
Returns:

List containing the gradients of the parameters.
Return type:

list
compute_normalization(space)[source]

Compute the normalization constant of the wavefunction.

Z_{\bm{\lambda}}= \sqrt{\sum_{\bm{\sigma}}|\psi_{\bm{\lambda\mu}}|^2}= \sqrt{\sum_{\bm{\sigma}} p_{\bm{\lambda}}(\bm{\sigma})}

Parameters:space (torch.Tensor) – A rank 2 tensor of the entire visible space.
device

The device that the model is on.

fit(data, epochs=100, pos_batch_size=100, neg_batch_size=None, k=1, lr=0.001, input_bases=None, progbar=False, starting_epoch=1, time=False, callbacks=None, optimizer=<class 'torch.optim.sgd.SGD'>, **kwargs)[source]

Train the WaveFunction.

Parameters:
  • data (np.array) – The training samples
  • epochs (int) – The number of full training passes through the dataset. Technically, this specifies the index of the last training epoch, which is relevant if starting_epoch is being set.
  • pos_batch_size (int) – The size of batches for the positive phase taken from the data.
  • neg_batch_size (int) – The size of batches for the negative phase taken from the data. Defaults to pos_batch_size.
  • k (int) – The number of contrastive divergence steps.
  • lr (float) – Learning rate
  • input_bases (np.array) – The measurement bases for each sample. Must be provided if training a ComplexWaveFunction.
  • progbar (bool or str) – Whether or not to display a progress bar. If “notebook” is passed, will use a Jupyter notebook compatible progress bar.
  • starting_epoch (int) – The epoch to start from. Useful if continuing training from a previous state.
  • callbacks (list[qucumber.callbacks.CallbackBase]) – Callbacks to run while training.
  • optimizer (torch.optim.Optimizer) – The constructor of a torch optimizer.
  • kwargs – Keyword arguments to pass to the optimizer
generate_hilbert_space(size=None, device=None)[source]

Generates Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space. Defaults to the number of visible units.
  • device – The device to create the Hilbert space matrix on. Defaults to the device this model is on.
Returns:

A tensor with all the basis states of the Hilbert space.
Return type:

torch.Tensor
gradient()[source]

Compute the gradient of a set of samples.

load(location)[source]

Loads the WaveFunction parameters from the given location ignoring any metadata stored in the file. Overwrites the WaveFunction’s parameters.

Note

The WaveFunction object on which this function is called must have the same parameter shapes as the one who’s parameters are being loaded.

Parameters:location (str or file) – The location to load the WaveFunction parameters from.
max_size

Maximum size of the Hilbert space for full enumeration

networks

A list of the names of the internal RBMs.

phase(v)[source]

Compute the phase of a given vector/matrix of visible states.

\text{phase}(\bm{\sigma})

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Matrix/vector containing the phases of v
Return type:torch.Tensor
probability(v, Z)[source]

Evaluates the probability of the given vector(s) of visible states.

Parameters:
Returns:

The probability of the given vector(s) of visible units.
Return type:

torch.Tensor
psi(v)[source]

Compute the (unnormalized) wavefunction of a given vector/matrix of visible states.

\psi(\bm{\sigma})

Parameters:v (torch.Tensor) – visible states \bm{\sigma}
Returns:Complex object containing the value of the wavefunction for each visible state
Return type:torch.Tensor
rbm_am

The RBM to be used to learn the wavefunction amplitude.

reinitialize_parameters()[source]

Randomize the parameters of the internal RBMs.

sample(k, num_samples=1, initial_state=None, overwrite=False)[source]

Performs k steps of Block Gibbs sampling. One step consists of sampling the hidden state \bm{h} from the conditional distribution p_{\bm{\lambda}}(\bm{h}\:|\:\bm{v}), and sampling the visible state \bm{v} from the conditional distribution p_{\bm{\lambda}}(\bm{v}\:|\:\bm{h}).

Parameters:
  • k (int) – Number of Block Gibbs steps.
  • num_samples (int) – The number of samples to generate.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided.
save(location, metadata=None)[source]

Saves the WaveFunction parameters to the given location along with any given metadata.

Parameters:
  • location (str or file) – The location to save the data.
  • metadata (dict) – Any extra metadata to store alongside the WaveFunction parameters.
stop_training

If True, will not train.

If this property is set to True during the training cycle, training will terminate once the current batch or epoch ends (depending on when stop_training was set).

subspace_vector(num, size=None, device=None)[source]

Generates a single vector from the Hilbert space of dimension 2^{\text{size}}.

Parameters:
  • size (int) – The size of each element of the Hilbert space.
  • num (int) – The specific vector to return from the Hilbert space. Since the Hilbert space can be represented by the set of binary strings of length size, num is equivalent to the decimal representation of the returned vector.
  • device – The device to create the vector on. Defaults to the device this model is on.
Returns:

A state from the Hilbert space.
Return type:

torch.Tensor

Callbacks

class qucumber.callbacks.CallbackBase[source]

Base class for callbacks.

on_batch_end(nn_state, epoch, batch)[source]

Called at the end of each batch.

Parameters:
on_batch_start(nn_state, epoch, batch)[source]

Called at the start of each batch.

Parameters:
on_epoch_end(nn_state, epoch)[source]

Called at the end of each epoch.

Parameters:
on_epoch_start(nn_state, epoch)[source]

Called at the start of each epoch.

Parameters:
on_train_end(nn_state)[source]

Called at the end of the training cycle.

Parameters:nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction being trained.
on_train_start(nn_state)[source]

Called at the start of the training cycle.

Parameters:nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction being trained.
class qucumber.callbacks.LambdaCallback(on_train_start=None, on_train_end=None, on_epoch_start=None, on_epoch_end=None, on_batch_start=None, on_batch_end=None)[source]

Class for creating simple callbacks.

This callback is constructed using the passed functions that will be called at the appropriate time.

Parameters:
  • on_train_start (callable or None) – A function to be called at the start of the training cycle. Must follow the same signature as CallbackBase.on_train_start.
  • on_train_end (callable or None) – A function to be called at the end of the training cycle. Must follow the same signature as CallbackBase.on_train_end.
  • on_epoch_start (callable or None) – A function to be called at the start of every epoch. Must follow the same signature as CallbackBase.on_epoch_start.
  • on_epoch_end (callable or None) – A function to be called at the end of every epoch. Must follow the same signature as CallbackBase.on_epoch_end.
  • on_batch_start (callable or None) – A function to be called at the start of every batch. Must follow the same signature as CallbackBase.on_batch_start.
  • on_batch_end (callable or None) – A function to be called at the end of every batch. Must follow the same signature as CallbackBase.on_batch_end.
class qucumber.callbacks.ModelSaver(period, folder_path, file_name, save_initial=True, metadata=None, metadata_only=False)[source]

Callback which allows model parameters (along with some metadata) to be saved to disk at regular intervals.

This callback is called at the end of each epoch. If save_initial is True, will also be called at the start of the training cycle.

Parameters:
  • period (int) – Frequency of model saving (in epochs).
  • folder_path (str) – The directory in which to save the files
  • file_name (str) – The name of the output files. Should be a format string with one blank, which will be filled with either the epoch number or the word “initial”.
  • save_initial (bool) – Whether to save the initial parameters (and metadata).
  • metadata (callable or dict or None) – The metadata to save to disk with the model parameters Can be either a function or a dictionary. In the case of a function, it must take 2 arguments the RBM being trained, and the current epoch number, and then return a dictionary containing the metadata to be saved.
  • metadata_only (bool) – Whether to save only the metadata to disk.
class qucumber.callbacks.Logger(period, logger_fn=<built-in function print>, msg_gen=None, **msg_gen_kwargs)[source]

Callback which logs output at regular intervals.

This callback is called at the end of each epoch.

Parameters:
  • period (int) – Logging frequency (in epochs).
  • logger_fn (callable) – The function used for logging. Must take 1 string as an argument. Defaults to the standard print function.
  • msg_gen (callable) – A callable which generates the string to be logged. Must take 2 positional arguments: the RBM being trained and the current epoch. It must also be able to take some keyword arguments.
  • **kwargs – Keyword arguments which will be passed to msg_gen.
class qucumber.callbacks.EarlyStopping(period, tolerance, patience, evaluator_callback, quantity_name)[source]

Stop training once the model stops improving. The specific criterion for stopping is:

\left\vert\frac{M_{t-p} - M_t}{M_{t-p}}\right\vert < \epsilon

where M_t is the metric value at the current evaluation (time t), p is the “patience” parameter, and \epsilon is the tolerance.

This callback is called at the end of each epoch.

Parameters:
  • period (int) – Frequency with which the callback checks whether training has converged (in epochs).
  • tolerance (float) – The maximum relative change required to consider training as having converged.
  • patience (int) – How many intervals to wait before claiming the training has converged.
  • evaluator_callback (MetricEvaluator or ObservableEvaluator) – An instance of MetricEvaluator or ObservableEvaluator which computes the metric that we want to check for convergence.
  • quantity_name (str) – The name of the metric/observable stored in evaluator_callback.
class qucumber.callbacks.VarianceBasedEarlyStopping(period, tolerance, patience, evaluator_callback, quantity_name, variance_name)[source]

Stop training once the model stops improving. This is a variation on the EarlyStopping class which takes the variance of the metric into account. The specific criterion for stopping is:

\left\vert\frac{M_{t-p} - M_t}{\sigma_{t-p}}\right\vert < \kappa

where M_t is the metric value at the current evaluation (time t), p is the “patience” parameter, \sigma_t is the variance of the metric, and \kappa is the tolerance.

This callback is called at the end of each epoch.

Parameters:
  • period (int) – Frequency with which the callback checks whether training has converged (in epochs).
  • tolerance (float) – The maximum (standardized) change required to consider training as having converged.
  • patience (int) – How many intervals to wait before claiming the training has converged.
  • evaluator_callback (MetricEvaluator or ObservableEvaluator) – An instance of MetricEvaluator or ObservableEvaluator which computes the metric/observable that we want to check for convergence.
  • quantity_name (str) – The name of the metric/obserable stored in evaluator_callback.
  • variance_name (str) – The name of the variance stored in evaluator_callback.
class qucumber.callbacks.MetricEvaluator(period, metrics, verbose=False, log=None, **metric_kwargs)[source]

Evaluate and hold on to the results of the given metric(s).

This callback is called at the end of each epoch.

Note

Since callbacks are given to fit as a list, they will be called in a deterministic order. It is therefore recommended that instances of MetricEvaluator be among the first callbacks in the list passed to fit, as one would often use it in conjunction with other callbacks like EarlyStopping which may depend on MetricEvaluator having been called.

Parameters:
  • period (int) – Frequency with which the callback evaluates the given metric(s).
  • metrics (dict(str, callable)) – A dictionary of callables where the keys are the names of the metrics and the callables take the WaveFunction being trained as their positional argument, along with some keyword arguments. The metrics are evaluated and put into an internal dictionary structure resembling the structure of metrics.
  • verbose (bool) – Whether to print metrics to stdout.
  • log (str) – A filepath to log metric values to in CSV format.
  • **metric_kwargs – Keyword arguments to be passed to metrics.
__getattr__(metric)[source]

Return an array of all recorded values of the given metric.

Parameters:metric (str) – The metric to retrieve.
Returns:The past values of the metric.
Return type:np.array
__len__()[source]

Return the number of timesteps that metrics have been evaluated for.

Return type:int
clear_history()[source]

Delete all metric values the instance is currently storing.

epochs

Return a list of all epochs that have been recorded.

Return type:np.array
get_value(name, index=None)[source]

Retrieve the value of the desired metric from the given timestep.

Parameters:
  • name (str) – The name of the metric to retrieve.
  • index (int or None) – The index/timestep from which to retrieve the metric. Negative indices are supported. If None, will just get the most recent value.
names

The names of the tracked metrics.

Return type:list[str]
class qucumber.callbacks.ObservableEvaluator(period, observables, verbose=False, log=None, **sampling_kwargs)[source]

Evaluate and hold on to the results of the given observable(s).

This callback is called at the end of each epoch.

Note

Since callback are given to fit as a list, they will be called in a deterministic order. It is therefore recommended that instances of ObservableEvaluator be among the first callbacks in the list passed to fit, as one would often use it in conjunction with other callbacks like EarlyStopping which may depend on ObservableEvaluator having been called.

Parameters:
  • period (int) – Frequency with which the callback evaluates the given observables(s).
  • observables (list(qucumber.observables.ObservableBase)) – A list of Observables. Observable statistics are evaluated by sampling the WaveFunction. Note that observables that have the same name will conflict, and precedence will be given to the right-most observable argument.
  • verbose (bool) – Whether to print metrics to stdout.
  • log (str) – A filepath to log metric values to in CSV format.
  • **sampling_kwargs – Keyword arguments to be passed to Observable.statistics. Ex. num_samples, num_chains, burn_in, steps.
__getattr__(observable)[source]

Return an ObservableStatistics containing recorded statistics of the given observable.

Parameters:observable (str) – The observable to retrieve.
Returns:The past values of the observable.
Return type:ObservableStatistics
__len__()[source]

Return the number of timesteps that observables have been evaluated for.

Return type:int
clear_history()[source]

Delete all statistics the instance is currently storing.

epochs

Return a list of all epochs that have been recorded.

Return type:np.array
get_value(name, index=None)[source]

Retrieve the statistics of the desired observable from the given timestep.

Parameters:
  • name (str) – The name of the observable to retrieve.
  • index (int or None) – The index/timestep from which to retrieve the observable. Negative indices are supported. If None, will just get the most recent value.
names

The names of the tracked observables.

Return type:list[str]
class qucumber.callbacks.LivePlotting(period, evaluator_callback, quantity_name, error_name=None, total_epochs=None, smooth=True)[source]

Plots metrics/observables.

This callback is called at the end of each epoch.

Parameters:
  • period (int) – Frequency with which the callback updates the plots (in epochs).
  • evaluator_callback (MetricEvaluator or ObservableEvaluator) – An instance of MetricEvaluator or ObservableEvaluator which computes the metric/observable that we want to plot.
  • quantity_name (str) – The name of the metric/observable stored in evaluator_callback.
  • error_name (str) – The name of the error stored in evaluator_callback.
class qucumber.callbacks.Timer(verbose=True)[source]

Callback which records the training time.

This callback is always called at the start and end of training. It will run at the end of an epoch or batch if the given model’s stop_training property is set to True.

Parameters:verbose (bool) – Whether to print the elapsed time at the end of training.

Observables

Pauli Operators

class qucumber.observables.SigmaZ[source]

Bases: qucumber.observables.ObservableBase

The \sigma_z observable.

Computes the magnetization in the Z direction of a spin chain.

apply(nn_state, samples)[source]

Computes the magnetization of each sample given a batch of samples.

Parameters:
name

The name of the Observable.

sample(nn_state, k, num_samples=1, initial_state=None, overwrite=False)[source]

Draws samples of the observable using the given WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • k (int) – The number of Gibbs Steps to perform before drawing a sample.
  • num_samples (int) – The number of samples to draw.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided, with the updated state of the Markov chain.
statistics(nn_state, num_samples, num_chains=0, burn_in=1000, steps=1)[source]

Estimates the expected value, variance, and the standard error of the observable over the distribution defined by the WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • num_samples (int) – The number of samples to draw. The actual number of samples drawn may be slightly higher if num_samples % num_chains != 0.
  • num_chains (int) – The number of Markov chains to run in parallel; if 0, will use a number of chains equal to num_samples.
  • burn_in (int) – The number of Gibbs Steps to perform before recording any samples.
  • steps (int) – The number of Gibbs Steps to take between each sample.
Returns:

A dictionary containing the (estimated) expected value (key: “mean”), variance (key: “variance”), and standard error (key: “std_error”) of the observable.
Return type:

dict(str, float)
statistics_from_samples(nn_state, samples)[source]

Estimates the expected value, variance, and the standard error of the observable using the given samples.

Parameters:
symbol

The algebraic symbol representing the Observable.

class qucumber.observables.SigmaX[source]

Bases: qucumber.observables.ObservableBase

The \sigma_x observable

Computes the magnetization in the X direction of a spin chain.

apply(nn_state, samples)[source]

Computes the magnetization along X of each sample in the given batch of samples.

Parameters:
name

The name of the Observable.

sample(nn_state, k, num_samples=1, initial_state=None, overwrite=False)[source]

Draws samples of the observable using the given WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • k (int) – The number of Gibbs Steps to perform before drawing a sample.
  • num_samples (int) – The number of samples to draw.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided, with the updated state of the Markov chain.
statistics(nn_state, num_samples, num_chains=0, burn_in=1000, steps=1)[source]

Estimates the expected value, variance, and the standard error of the observable over the distribution defined by the WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • num_samples (int) – The number of samples to draw. The actual number of samples drawn may be slightly higher if num_samples % num_chains != 0.
  • num_chains (int) – The number of Markov chains to run in parallel; if 0, will use a number of chains equal to num_samples.
  • burn_in (int) – The number of Gibbs Steps to perform before recording any samples.
  • steps (int) – The number of Gibbs Steps to take between each sample.
Returns:

A dictionary containing the (estimated) expected value (key: “mean”), variance (key: “variance”), and standard error (key: “std_error”) of the observable.
Return type:

dict(str, float)
statistics_from_samples(nn_state, samples)[source]

Estimates the expected value, variance, and the standard error of the observable using the given samples.

Parameters:
symbol

The algebraic symbol representing the Observable.

class qucumber.observables.SigmaY[source]

Bases: qucumber.observables.ObservableBase

The \sigma_y observable

Computes the magnetization in the Y direction of a spin chain.

apply(nn_state, samples)[source]

Computes the magnetization along Y of each sample in the given batch of samples.

Parameters:
name

The name of the Observable.

sample(nn_state, k, num_samples=1, initial_state=None, overwrite=False)[source]

Draws samples of the observable using the given WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • k (int) – The number of Gibbs Steps to perform before drawing a sample.
  • num_samples (int) – The number of samples to draw.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided, with the updated state of the Markov chain.
statistics(nn_state, num_samples, num_chains=0, burn_in=1000, steps=1)[source]

Estimates the expected value, variance, and the standard error of the observable over the distribution defined by the WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • num_samples (int) – The number of samples to draw. The actual number of samples drawn may be slightly higher if num_samples % num_chains != 0.
  • num_chains (int) – The number of Markov chains to run in parallel; if 0, will use a number of chains equal to num_samples.
  • burn_in (int) – The number of Gibbs Steps to perform before recording any samples.
  • steps (int) – The number of Gibbs Steps to take between each sample.
Returns:

A dictionary containing the (estimated) expected value (key: “mean”), variance (key: “variance”), and standard error (key: “std_error”) of the observable.
Return type:

dict(str, float)
statistics_from_samples(nn_state, samples)[source]

Estimates the expected value, variance, and the standard error of the observable using the given samples.

Parameters:
symbol

The algebraic symbol representing the Observable.

Neighbour Interactions

class qucumber.observables.NeighbourInteraction(periodic_bcs=False, c=1)[source]

Bases: qucumber.observables.ObservableBase

The \sigma^z_i \sigma^z_{i+c} observable

Computes the c-th nearest neighbour interaction for a spin chain with either open or periodic boundary conditions.

Parameters:
  • periodic_bcs (bool) – Specifies whether the system has periodic boundary conditions.
  • c (int) – Interaction distance.
apply(nn_state, samples)[source]

Computes the energy of this neighbour interaction for each sample given a batch of samples.

Parameters:
name

The name of the Observable.

sample(nn_state, k, num_samples=1, initial_state=None, overwrite=False)[source]

Draws samples of the observable using the given WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • k (int) – The number of Gibbs Steps to perform before drawing a sample.
  • num_samples (int) – The number of samples to draw.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided, with the updated state of the Markov chain.
statistics(nn_state, num_samples, num_chains=0, burn_in=1000, steps=1)[source]

Estimates the expected value, variance, and the standard error of the observable over the distribution defined by the WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • num_samples (int) – The number of samples to draw. The actual number of samples drawn may be slightly higher if num_samples % num_chains != 0.
  • num_chains (int) – The number of Markov chains to run in parallel; if 0, will use a number of chains equal to num_samples.
  • burn_in (int) – The number of Gibbs Steps to perform before recording any samples.
  • steps (int) – The number of Gibbs Steps to take between each sample.
Returns:

A dictionary containing the (estimated) expected value (key: “mean”), variance (key: “variance”), and standard error (key: “std_error”) of the observable.
Return type:

dict(str, float)
statistics_from_samples(nn_state, samples)[source]

Estimates the expected value, variance, and the standard error of the observable using the given samples.

Parameters:
symbol

The algebraic symbol representing the Observable.

Abstract Observable

Note

This is an Abstract Base Class, it is not meant to be used directly. The following API reference is mostly for developers.

class qucumber.observables.ObservableBase[source]

Bases: abc.ABC

Base class for observables.

apply(nn_state, samples)[source]

Computes the value of the observable, row-wise, on a batch of samples. Must be implemented by any subclasses.

Parameters:
name

The name of the Observable.

sample(nn_state, k, num_samples=1, initial_state=None, overwrite=False)[source]

Draws samples of the observable using the given WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • k (int) – The number of Gibbs Steps to perform before drawing a sample.
  • num_samples (int) – The number of samples to draw.
  • initial_state (torch.Tensor) – The initial state of the Markov Chain. If given, num_samples will be ignored.
  • overwrite (bool) – Whether to overwrite the initial_state tensor, if it is provided, with the updated state of the Markov chain.
statistics(nn_state, num_samples, num_chains=0, burn_in=1000, steps=1)[source]

Estimates the expected value, variance, and the standard error of the observable over the distribution defined by the WaveFunction.

Parameters:
  • nn_state (qucumber.nn_states.WaveFunctionBase) – The WaveFunction to draw samples from.
  • num_samples (int) – The number of samples to draw. The actual number of samples drawn may be slightly higher if num_samples % num_chains != 0.
  • num_chains (int) – The number of Markov chains to run in parallel; if 0, will use a number of chains equal to num_samples.
  • burn_in (int) – The number of Gibbs Steps to perform before recording any samples.
  • steps (int) – The number of Gibbs Steps to take between each sample.
Returns:

A dictionary containing the (estimated) expected value (key: “mean”), variance (key: “variance”), and standard error (key: “std_error”) of the observable.
Return type:

dict(str, float)
statistics_from_samples(nn_state, samples)[source]

Estimates the expected value, variance, and the standard error of the observable using the given samples.

Parameters:
symbol

The algebraic symbol representing the Observable.

Complex Algebra

qucumber.utils.cplx.absolute_value(x)[source]

Computes the complex absolute value elementwise.

Parameters:x (torch.Tensor) – A complex tensor.
Returns:A real tensor.
Return type:torch.Tensor
qucumber.utils.cplx.conjugate(x)[source]

A function that takes the conjugate transpose of the argument.

Parameters:x (torch.Tensor) – A complex vector or matrix.
Returns:The conjugate of x.
Return type:torch.Tensor
qucumber.utils.cplx.elementwise_division(x, y)[source]

Elementwise division of x by y.

Parameters:
Return type:

torch.Tensor
qucumber.utils.cplx.elementwise_mult(x, y)[source]

Alias for scalar_mult().

qucumber.utils.cplx.inner_prod(x, y)[source]

A function that returns the inner product of two complex vectors, x and y (<x|y>).

Parameters:
Raises:

ValueError – If x and y are not complex vectors with their first dimensions being 2, then the function will not execute.
Returns:

The inner product, \langle x\vert y\rangle.
Return type:

torch.Tensor
qucumber.utils.cplx.kronecker_prod(x, y)[source]

A function that returns the tensor / kronecker product of 2 complex tensors, x and y.

Parameters:
Raises:

ValueError – If x and y do not have 3 dimensions or their first dimension is not 2, the function cannot execute.
Returns:

The tensorproduct of x and y, x \otimes y.
Return type:

torch.Tensor
qucumber.utils.cplx.make_complex(x, y=None)[source]

A function that combines the real (x) and imaginary (y) parts of a vector or a matrix.

Note

x and y must have the same shape. Also, this will not work for rank zero tensors.

Parameters:
  • x (torch.Tensor) – The real part
  • y (torch.Tensor) – The imaginary part. Can be None, in which case, the resulting complex tensor will have imaginary part equal to zero.
Returns:

The tensor [x,y] = x + yi.
Return type:

torch.Tensor
qucumber.utils.cplx.matmul(x, y)[source]

A function that computes complex matrix-matrix and matrix-vector products.

Note

If one wishes to do matrix-vector products, the vector must be the second argument (y).

Parameters:
Returns:

The product between x and y.
Return type:

torch.Tensor
qucumber.utils.cplx.norm(x)[source]

A function that returns the norm of the argument.

Parameters:x (torch.Tensor) – A complex scalar.
Returns:|x|.
Return type:torch.Tensor
qucumber.utils.cplx.norm_sqr(x)[source]

A function that returns the squared norm of the argument.

Parameters:x (torch.Tensor) – A complex scalar.
Returns:|x|^2.
Return type:torch.Tensor
qucumber.utils.cplx.outer_prod(x, y)[source]

A function that returns the outer product of two complex vectors, x and y.

Parameters:
Raises:

ValueError – If x and y are not complex vectors with their first dimensions being 2, then the function will not execute.
Returns:

The outer product between x and y, \vert x \rangle\langle y\vert.
Return type:

torch.Tensor
qucumber.utils.cplx.scalar_divide(x, y)[source]

A function that computes the division of x by y.

Parameters:
  • x (torch.Tensor) – The numerator (a complex scalar, vector or matrix).
  • y (torch.Tensor) – The denominator (a complex scalar).
Returns:

x / y
Return type:

torch.Tensor
qucumber.utils.cplx.scalar_mult(x, y, out=None)[source]

A function that computes the product between complex matrices and scalars, complex vectors and scalars or two complex scalars.

Parameters:
  • x (torch.Tensor) – A complex scalar, vector or matrix.
  • y (torch.Tensor) – A complex scalar, vector or matrix.
  • z (torch.Tensor) – The complex tensor to write the output to.
  • z – A complex scalar, vector or matrix. Can be None, in which case, a new tensor is created and returned. Otherwise, the method overwrites z.
Returns:

The product between x and y. Either overwrites z, or returns a new tensor.
Return type:

torch.Tensor

Data Handling

qucumber.utils.data.extract_refbasis_samples(train_samples, train_bases)[source]

Extract the reference basis samples from the data.

Parameters:
  • train_samples (numpy.array) – The training samples.
  • train_bases (numpy.array) – The bases of the training samples.
Returns:

The samples in the data that are only in the reference basis.
Return type:

torch.Tensor
qucumber.utils.data.load_data(tr_samples_path, tr_psi_path=None, tr_bases_path=None, bases_path=None)[source]

Load the data required for training.

Parameters:
  • tr_samples_path (str) – The path to the training data.
  • tr_psi_path (str) – The path to the target/true wavefunction.
  • tr_bases_path (str) – The path to the basis data.
  • bases_path (str) – The path to a file containing all possible bases used in the tr_bases_path file.
Returns:

A list of all input parameters.
Return type:

list

Indices and tables