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@josh146 josh146 released this 27 Nov 18:18
· 2998 commits to master since this release
v0.13.0
15a61bb

New features since last release

Automatically optimize the number of measurements

  • QNodes in tape mode now support returning observables on the same wire whenever the observables are qubit-wise commuting Pauli words. Qubit-wise commuting observables can be evaluated with a single device run as they are diagonal in the same basis, via a shared set of single-qubit rotations. (#882)

    The following example shows a single QNode returning the expectation values of the qubit-wise commuting Pauli words XX and XI:

    qml.enable_tape()

@qml.qnode(dev)
def f(x):
    qml.Hadamard(wires=0)
    qml.Hadamard(wires=1)
    qml.CRot(0.1, 0.2, 0.3, wires=[1, 0])
    qml.RZ(x, wires=1)
    return qml.expval(qml.PauliX(0) @ qml.PauliX(1)), qml.expval(qml.PauliX(0))
    >>> f(0.4)
tensor([0.89431013, 0.9510565 ], requires_grad=True)

  • The ExpvalCost class (previously VQECost) now provides observable optimization using the optimize argument, resulting in potentially fewer device executions. (#902)

    This is achieved by separating the observables composing the Hamiltonian into qubit-wise commuting groups and evaluating those groups on a single QNode using functionality from the qml.grouping module:

    qml.enable_tape()
commuting_obs = [qml.PauliX(0), qml.PauliX(0) @ qml.PauliZ(1)]
H = qml.vqe.Hamiltonian([1, 1], commuting_obs)

dev = qml.device("default.qubit", wires=2)
ansatz = qml.templates.StronglyEntanglingLayers

cost_opt = qml.ExpvalCost(ansatz, H, dev, optimize=True)
cost_no_opt = qml.ExpvalCost(ansatz, H, dev, optimize=False)

params = qml.init.strong_ent_layers_uniform(3, 2)

    Grouping these commuting observables leads to fewer device executions:

    >>> cost_opt(params)
>>> ex_opt = dev.num_executions
>>> cost_no_opt(params)
>>> ex_no_opt = dev.num_executions - ex_opt
>>> print("Number of executions:", ex_no_opt)
Number of executions: 2
>>> print("Number of executions (optimized):", ex_opt)
Number of executions (optimized): 1

New quantum gradient features

  • Compute the analytic gradient of quantum circuits in parallel on supported devices. (#840)

    This release introduces support for batch execution of circuits, via a new device API method Device.batch_execute(). Devices that implement this new API support submitting a batch of circuits for parallel evaluation simultaneously, which can significantly reduce the computation time.

    Furthermore, if using tape mode and a compatible device, gradient computations will automatically make use of the new batch API---providing a speedup during optimization.

  • Gradient recipes are now much more powerful, allowing for operations to define their gradient via an arbitrary linear combination of circuit evaluations. (#909) (#915)

    With this change, gradient recipes can now be of the form \frac{\partial}{\partial\phi_k}f(\phi_k) = \sum_{i} c_i f(a_i \phi_k + s_i ), and are no longer restricted to two-term shifts with identical (but opposite in sign) shift values.

    As a result, PennyLane now supports native analytic quantum gradients for the controlled rotation operations CRX, CRY, CRZ, and CRot. This allows for parameter-shift analytic gradients on hardware, without decomposition.

    Note that this is a breaking change for developers; please see the Breaking Changes section for more details.

  • The qnn.KerasLayer class now supports differentiating the QNode through classical backpropagation in tape mode. (#869)

    qml.enable_tape()

dev = qml.device("default.qubit.tf", wires=2)

@qml.qnode(dev, interface="tf", diff_method="backprop")
def f(inputs, weights):
    qml.templates.AngleEmbedding(inputs, wires=range(2))
    qml.templates.StronglyEntanglingLayers(weights, wires=range(2))
    return [qml.expval(qml.PauliZ(i)) for i in range(2)]

weight_shapes = {"weights": (3, 2, 3)}

qlayer = qml.qnn.KerasLayer(f, weight_shapes, output_dim=2)

inputs = tf.constant(np.random.random((4, 2)), dtype=tf.float32)

with tf.GradientTape() as tape:
    out = qlayer(inputs)

tape.jacobian(out, qlayer.trainable_weights)

New operations, templates, and measurements

  • Adds the qml.density_matrix QNode return with partial trace capabilities. (#878)

    The density matrix over the provided wires is returned, with all other subsystems traced out. qml.density_matrix currently works for both the default.qubit and default.mixed devices.

    qml.enable_tape()
dev = qml.device("default.qubit", wires=2)

def circuit(x):
    qml.PauliY(wires=0)
    qml.Hadamard(wires=1)
    return qml.density_matrix(wires=[1])  # wire 0 is traced out

  • Adds the square-root X gate SX. (#871)

    dev = qml.device("default.qubit", wires=1)

@qml.qnode(dev)
def circuit():
    qml.SX(wires=[0])
    return qml.expval(qml.PauliZ(wires=[0]))

  • Two new hardware-efficient particle-conserving templates have been implemented to perform VQE-based quantum chemistry simulations. The new templates apply several layers of the particle-conserving entanglers proposed in Figs. 2a and 2b of Barkoutsos et al., arXiv:1805.04340 (#875) (#876)

Estimate and track resources

  • The QuantumTape class now contains basic resource estimation functionality. The method tape.get_resources() returns a dictionary with a list of the constituent operations and the number of times they appear in the circuit. Similarly, tape.get_depth() computes the circuit depth. (#862)

    >>> with qml.tape.QuantumTape() as tape:
...    qml.Hadamard(wires=0)
...    qml.RZ(0.26, wires=1)
...    qml.CNOT(wires=[1, 0])
...    qml.Rot(1.8, -2.7, 0.2, wires=0)
...    qml.Hadamard(wires=1)
...    qml.CNOT(wires=[0, 1])
...    qml.expval(qml.PauliZ(0) @ qml.PauliZ(1))
>>> tape.get_resources()
{'Hadamard': 2, 'RZ': 1, 'CNOT': 2, 'Rot': 1}
>>> tape.get_depth()
4

  • The number of device executions over a QNode's lifetime can now be returned using num_executions. (#853)

    >>> dev = qml.device("default.qubit", wires=2)
>>> @qml.qnode(dev)
... def circuit(x, y):
...    qml.RX(x, wires=[0])
...    qml.RY(y, wires=[1])
...    qml.CNOT(wires=[0, 1])
...    return qml.expval(qml.PauliZ(0) @ qml.PauliX(1))
>>> for _ in range(10):
...    circuit(0.432, 0.12)
>>> print(dev.num_executions)
10

Improvements

  • Support for tape mode has improved across PennyLane. The following features now work in tape mode:

  • A new function, qml.refresh_devices(), has been added, allowing PennyLane to rescan installed PennyLane plugins and refresh the device list. In addition, the qml.device loader will attempt to refresh devices if the required plugin device cannot be found. This will result in an improved experience if installing PennyLane and plugins within a running Python session (for example, on Google Colab), and avoid the need to restart the kernel/runtime. (#907)

  • When using grad_fn = qml.grad(cost) to compute the gradient of a cost function with the Autograd interface, the value of the intermediate forward pass is now available via the grad_fn.forward property (#914):

    def cost_fn(x, y):
    return 2 * np.sin(x[0]) * np.exp(-x[1]) + x[0] ** 3 + np.cos(y)

params = np.array([0.1, 0.5], requires_grad=True)
data = np.array(0.65, requires_grad=False)
grad_fn = qml.grad(cost_fn)

grad_fn(params, data)  # perform backprop and evaluate the gradient
grad_fn.forward  # the cost function value

  • Gradient-based optimizers now have a step_and_cost method that returns both the next step as well as the objective (cost) function output. (#916)

    >>> opt = qml.GradientDescentOptimizer()
>>> params, cost = opt.step_and_cost(cost_fn, params)

  • PennyLane provides a new experimental module qml.proc which provides framework-agnostic processing functions for array and tensor manipulations. (#886)

    Given the input tensor-like object, the call is dispatched to the corresponding array manipulation framework, allowing for end-to-end differentiation to be preserved.

    >>> x = torch.tensor([1., 2.])
>>> qml.proc.ones_like(x)
tensor([1, 1])
>>> y = tf.Variable([[0], [5]])
>>> qml.proc.ones_like(y, dtype=np.complex128)
<tf.Tensor: shape=(2, 1), dtype=complex128, numpy=
array([[1.+0.j],
       [1.+0.j]])>

    Note that these functions are experimental, and only a subset of common functionality is supported. Furthermore, the names and behaviour of these functions may differ from similar functions in common frameworks; please refer to the function docstrings for more details.

  • The gradient methods in tape mode now fully separate the quantum and classical processing. Rather than returning the evaluated gradients directly, they now return a tuple containing the required quantum and classical processing steps. (#840)

    def gradient_method(idx, param, **options):
    # generate the quantum tapes that must be computed
    # to determine the quantum gradient
    tapes = quantum_gradient_tapes(self)

    def processing_fn(results):
        # perform classical processing on the evaluated tapes
        # returning the evaluated quantum gradient
        return classical_processing(results)

    return tapes, processing_fn

    The JacobianTape.jacobian() method has been similarly modified to accumulate all gradient quantum tapes and classical processing functions, evaluate all quantum tapes simultaneously, and then apply the post-processing functions to the evaluated tape results.

  • The MultiRZ gate now has a defined generator, allowing it to be used in quantum natural gradient optimization. (#912)

  • The CRot gate now has a decomposition method, which breaks the gate down into rotations and CNOT gates. This allows CRot to be used on devices that do not natively support it. (#908)

  • The classical processing in the MottonenStatePreparation template has been largely rewritten to use dense matrices and tensor manipulations wherever possible. This is in preparation to support differentiation through the template in the future. (#864)

  • Device-based caching has replaced QNode caching. Caching is now accessed by passing a cache argument to the device. (#851)

    The cache argument should be an integer specifying the size of the cache. For example, a cache of size 10 is created using:

    >>> dev = qml.device("default.qubit", wires=2, cache=10)

  • The Operation, Tensor, and MeasurementProcess classes now have the __copy__ special method defined. (#840)

    This allows us to ensure that, when a shallow copy is performed of an operation, the mutable list storing the operation parameters is also shallow copied. Both the old operation and the copied operation will continue to share the same parameter data,

    >>> import copy
>>> op = qml.RX(0.2, wires=0)
>>> op2 = copy.copy(op)
>>> op.data[0] is op2.data[0]
True

    however the list container is not a reference:

    >>> op.data is op2.data
False

    This allows the parameters of the copied operation to be modified, without mutating the parameters of the original operation.

  • The QuantumTape.copy method has been tweaked so that (#840):

    • Optionally, the tape's operations are shallow copied in addition to the tape by passing the copy_operations=True boolean flag. This allows the copied tape's parameters to be mutated without affecting the original tape's parameters. (Note: the two tapes will share parameter data until one of the tapes has their parameter list modified.)

    • Copied tapes can be cast to another QuantumTape subclass by passing the tape_cls keyword argument.

Breaking changes

  • Updated how parameter-shift gradient recipes are defined for operations, allowing for gradient recipes that are specified as an arbitrary number of terms. (#909)

    Previously, Operation.grad_recipe was restricted to two-term parameter-shift formulas. With this change, the gradient recipe now contains elements of the form [c_i, a_i, s_i], resulting in a gradient recipe of \frac{\partial}{\partial\phi_k}f(\phi_k) = \sum_{i} c_i f(a_i \phi_k + s_i ).

    As this is a breaking change, all custom operations with defined gradient recipes must be updated to continue working with PennyLane 0.13. Note though that if grad_recipe = None, the default gradient recipe remains unchanged, and corresponds to the two terms [c_0, a_0, s_0]=[1/2, 1, \pi/2] and [c_1, a_1, s_1]=[-1/2, 1, -\pi/2] for every parameter.

  • The VQECost class has been renamed to ExpvalCost to reflect its general applicability beyond VQE. Use of VQECost is still possible but will result in a deprecation warning. (#913)

Bug fixes

  • The default.qubit.tf device is updated to handle TensorFlow objects (e.g., tf.Variable) as gate parameters correctly when using the MultiRZ and CRot operations. (#921)

  • PennyLane tensor objects are now unwrapped in BaseQNode when passed as a keyword argument to the quantum function. (#903) (#893)

  • The new tape mode now prevents multiple observables from being evaluated on the same wire if the observables are not qubit-wise commuting Pauli words. (#882)

  • Fixes a bug in default.qubit whereby inverses of common gates were not being applied via efficient gate-specific methods, instead falling back to matrix-vector multiplication. The following gates were affected: PauliX, PauliY, PauliZ, Hadamard, SWAP, S, T, CNOT, CZ. (#872)

  • The PauliRot operation now gracefully handles single-qubit Paulis, and all-identity Paulis (#860).

  • Fixes a bug whereby binary Python operators were not properly propagating the requires_grad attribute to the output tensor. (#889)

  • Fixes a bug which prevents TorchLayer from doing backward when CUDA is enabled. (#899)

  • Fixes a bug where multi-threaded execution of QNodeCollection sometimes fails because of simultaneous queuing. This is fixed by adding thread locking during queuing. (#910)

  • Fixes a bug in QuantumTape.set_parameters(). The previous implementation assumed that the self.trainable_parms set would always be iterated over in increasing integer order. However, this is not guaranteed behaviour, and can lead to the incorrect tape parameters being set if this is not the case. (#923)

  • Fixes broken error message if a QNode is instantiated with an unknown exception. (#930)

Contributors

This release contains contributions from (in alphabetical order):

Juan Miguel Arrazola, Thomas Bromley, Christina Lee, Alain Delgado Gran, Olivia Di Matteo, Anthony Hayes, Theodor Isacsson, Josh Izaac, Soran Jahangiri, Nathan Killoran, Shumpei Kobayashi, Romain Moyard, Zeyue Niu, Maria Schuld, Antal Száva.

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