Interfaces
Circuit(...) returns a different type of circuit depending on its interface=
argument, which you set explicitly, as in PennyLane. Both interfaces run the same
CircuitSpec on the same providers. They differ only in how you pass the
weights and how you get gradients:
"numpy", the default, is the core circuit, which does not depend on any framework. You pass theweightsat every call, and the gradients come fromcircuit.jacobian(...). It does not use PyTorch, andpip install eigenkitwith no extra is enough."torch"is atorch.nn.Modulethat stores its weights as annn.Parameterand computes gradients throughtorch.autograd. It is part of the optional PyTorch package (thetorchextra).
numpy (default) |
torch |
|
|---|---|---|
| Returns | A core.circuit.Circuit. |
A TorchCircuit, which is an nn.Module. |
| Weights | They are passed at each call: circuit(weights, x). |
The circuit stores them as an nn.Parameter: circuit(x). |
| Gradients | circuit.jacobian(weights, x). |
loss.backward(), through autograd. |
| Dependency | The core (NumPy and SciPy). | The torch extra. |
| Best for | Chemistry and optimisation, variational loops, and custom training without a framework. | Hybrid quantum-classical models trained end to end in PyTorch. |
Both accept the same provider= argument, in any of its forms. See
Providers.
Circuit is a function, not a class
The top-level Circuit(...) is a factory function. It returns one of two
concrete types, depending on interface=: the NumPy circuit
eigenkit.core.circuit.Circuit, or the PyTorch circuit TorchCircuit, which is
an nn.Module. So it is not a class: isinstance(obj, Circuit),
issubclass(...), subclassing Circuit, and using Circuit as a type
annotation do not work. Check the type against the concrete class, or subclass
it, instead (from eigenkit.core.circuit import Circuit as NumpyCircuit, or
from eigenkit.torch import TorchCircuit).
The NumPy interface (default)
Circuit(blocks, observables) returns the core NumPy circuit. It does not store
parameters: you pass a 1-D weights vector, of length circuit.spec.n_weights, and
an inputs vector at each call.
import numpy as np
from eigenkit import Circuit, Encoding, Variational, all_z
circuit = Circuit(
blocks=[Encoding(in_features=4, rotation="RX"), Variational(depth=2)],
observables=all_z(4),
) # provider="numpy", interface="numpy"
weights = np.zeros(circuit.spec.n_weights)
x = np.array([0.1, 0.2, 0.3, 0.4])
y = circuit(weights, x) # shape (4,): one expectation per observable
Forward calls and batching
inputs can be 1-D, for a single sample, or 2-D, with shape (batch, n_inputs).
weights stays 1-D, because the weights are shared across the batch. The output has
shape (n_observables,) or (batch, n_observables). It becomes a scalar, or shape
(batch,), when a single observable is measured.
Gradients with circuit.jacobian
The NumPy interface is fully differentiable without PyTorch:
g = circuit.jacobian(weights, x) # d<O>/d(weights)
gw, gx = circuit.jacobian(weights, x, input_grad=True) # also d<O>/d(inputs)
jacobian returns shape (n_weights,) for a single observable, and
(n_observables, n_weights) for several, in the same way as __call__. It uses the
differentiation of the active backend when there is one, such as the analytic
adjoint method of the NumPy simulator, or the automatic differentiation of
PennyLane. Otherwise, it uses the parameter-shift rule, which works on any
backend. Pass one 1-D sample. For a batch, loop over the rows. On a hardware backend,
it raises an error, like .backward(), unless the configuration of the device sets
enable_gradients=True.
The variational optimisation tools use this gradient, so a loop that finds a ground
state takes a few lines and does not need PyTorch. These tools work on a purely
variational circuit, which has no inputs, so the example takes an ansatz in place
of the encoding circuit above:
from eigenkit import Variational, Z, minimize_expectation
ansatz = Circuit([Variational(depth=2)], observables=Z(0)) # n_inputs == 0
rng = np.random.default_rng(0)
x0 = rng.uniform(0, 2 * np.pi, size=ansatz.spec.n_weights)
result = minimize_expectation(ansatz, initial_parameters=x0)
print(result.optimal_value)
Other primitives
zero_state_probability(weights, inputs), which gives the fidelity used to invert
kernels, and probabilities(weights, inputs), which gives the whole distribution of
measurement outcomes, take the same (weights, inputs) arguments:
A circuit with no trainable weights, such as the inversion circuit of a kernel that
uses only data, takes an empty weight vector: inversion.zero_state_probability([], x).
When to use it
The NumPy interface is the right default for the domains that do not use a framework
(chemistry, optimization), for variational loops driven by SciPy, for any custom
training where you control the optimiser, and for light installs that should not
install PyTorch.
The PyTorch interface
Pass interface="torch" to get a torch.nn.Module. It stores its weights as an
nn.Parameter, so you call it with the inputs only, and you train it with any
PyTorch optimiser. It needs the torch extra, and it runs on the built-in NumPy
simulator, which is differentiable:
import torch
from eigenkit import Circuit, Encoding, Variational, all_z
layer = Circuit(
blocks=[Encoding(in_features=4), Variational(depth=2)],
observables=all_z(4),
interface="torch",
init=None, # optional initial weights, shape (n_weights,)
)
layer.weights # nn.Parameter of shape (n_weights,)
list(layer.parameters()) # plugs into torch.optim like any module
init sets the initial weight tensor. When it is not given, the weights are drawn
at random with torch.randn. Both the top-level Circuit(...) factory and a
TorchCircuit(...) built directly default to provider="numpy".
What the layer exposes
| Member | What it does |
|---|---|
layer(x) |
The forward pass. x can be 1-D (one sample) or 2-D, with shape (batch, n_inputs). |
weights |
The trainable nn.Parameter, of shape (n_weights,). |
spec, n_qubits, out_features |
The assembled CircuitSpec, and the two sizes derived from it. |
draw(decimals=3) |
A drawing of the circuit as text, over several lines. It takes no input, because the layer stores its weights. |
draw_mpl(**kwargs) |
The same drawing as a matplotlib (fig, ax). It needs the viz extra. |
zero_state_probability(x) |
The probability of the all-zeros outcome, which is the fidelity that the kernels use. |
submit(x) |
Submits the circuit without waiting, and returns a JobHandle. It works on Braket, Qiskit Runtime and IQM only. |
dry_run_info() |
Gives, without submitting anything, the gate counts, the shots and the number of circuits that a call runs. It works on Braket, Qiskit Runtime and IQM, and the other backends raise NotImplementedError. |
with_provider(provider, ...) |
Builds the same circuit again on another backend. See below. |
probabilities() and jacobian() are not available on the PyTorch circuit. The
whole distribution of measurement outcomes is a primitive of the NumPy interface,
and the gradients come from loss.backward() instead of a call to a jacobian.
submit() and dry_run_info() are explained in QPU and Cloud.
Forward calls and batching
A 1-D input is a single sample, and a 2-D input is a batch. The weights are shared across the batch, exactly as in the NumPy interface.
Gradients with loss.backward()
The gradients flow through torch.autograd:
x = torch.randn(8, 4)
target = torch.zeros(8, 4)
opt = torch.optim.Adam(layer.parameters(), lr=0.05)
loss = (layer(x) - target).pow(2).mean()
loss.backward() # weights.grad is populated
opt.step()
Backends with their own automatic differentiation, such as PennyLane, differentiate
through their own engine. For the other backends, the forward pass is wrapped in a
torch.autograd.Function, whose backward pass uses the same parameter-shift or
adjoint jacobian as the NumPy interface. Backends without gradients
(gradient_method="none", for example quantum hardware and Qiskit Runtime) raise a
clear error on .backward(). See QPU and Cloud for the pattern of training
on a simulator and then running on the device, and for enable_gradients=True, which
lets a hardware configuration use the parameter-shift rule on the device.
Training also works on the default NumPy provider, without PennyLane. The
analytic adjoint method of the NumPy backend differentiates a whole batch in one
sweep, so Circuit(..., interface="torch"), with the NumPy provider by default,
trains hybrid models efficiently. Switch to provider="pennylane" if you prefer its
simulator. Both process batches natively: the forward and backward passes of a
(B, …) batch run in one call, not in a Python loop over the samples.
Moving a circuit to another provider with with_provider
with_provider builds the same CircuitSpec and observables again on a
different backend, without listing the blocks again:
fast = layer.with_provider("qiskit") # clones weights
fresh = layer.with_provider("qiskit", copy_weights=False) # re-initialises
exact = layer.with_provider(
"qiskit",
init=torch.zeros(layer.spec.n_weights, dtype=torch.float64),
)
The weights are cloned by default. copy_weights=False draws new random weights, and
init= sets them explicitly (it takes precedence over copy_weights). The new layer
takes its data type from init, so pass dtype=torch.float64 to keep the double
precision that a layer built from blocks starts with. A plain torch.zeros(n) is
float32, and it would halve the precision without any warning.
Composing and saving
Because it is a plain nn.Module, a PyTorch circuit can be used inside
nn.Sequential and next to the ready-made layers (see Layers). The scikit-learn compatible estimators (HQNC, HQNR and
others) are built on it. Its state can be saved and restored with the usual PyTorch
methods (state_dict() and load_state_dict()), and fitted estimators are saved as
.eigenkit bundles. See Model persistence.
When to use it
Use the PyTorch interface when the quantum circuit is one layer in a larger PyTorch model, or whenever you want to train end to end with automatic differentiation and the optimisers and tools of PyTorch.
Same circuit, both interfaces
The interface is a choice made when the code runs, over one definition of the circuit. The blocks, the observables and the numerical results of the provider are the same:
import numpy as np, torch
from eigenkit import Circuit, Encoding, Variational, all_z
blocks = [Encoding(in_features=2), Variational(depth=1)]
np_circuit = Circuit(blocks, all_z(2)) # numpy
tc = Circuit(blocks, all_z(2), interface="torch") # torch
w = tc.weights.detach().numpy()
x = np.array([0.3, -0.2])
np.allclose(np_circuit(w, x), tc(torch.tensor(x)).detach().numpy()) # True
API reference
The factory function that chooses the type from interface=, and the two concrete
types that it returns.
eigenkit.circuit.Circuit(blocks, observables=None, provider='numpy', interface='numpy', init=None)
Build a circuit and compile it for a backend.
This is the entry point for the rest of the library: you give it blocks, and it
returns a circuit that you can call. The type of the circuit depends on
interface. The NumPy interface returns a core Circuit, and the PyTorch
interface returns a TorchCircuit.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
blocks
|
_BlocksOrSpec
|
The circuit. It can be a list of blocks to assemble, a |
required |
observables
|
ObservableLike
|
What to measure. |
None
|
provider
|
ProviderSpec
|
The backend that runs the circuit. It can be a registered name
( |
'numpy'
|
interface
|
_Interface
|
|
'numpy'
|
init
|
Tensor | None
|
The initial weights of the PyTorch circuit, of
shape |
None
|
Returns:
| Name | Type | Description |
|---|---|---|
circuit |
Circuit | TorchCircuit
|
The circuit for the requested |
Raises:
| Type | Description |
|---|---|
ValueError
|
If |
eigenkit.core.circuit.Circuit
A compiled circuit, ready to evaluate.
It holds a CircuitSpec, the observables to measure and a compiled backend
handle. The circuit is compiled once, when the instance is created, and every
call reuses the compiled handle. The instance does not store weights: you pass
the weights at each call.
This is the NumPy interface. The top-level Circuit(...) function of the
package returns this class for interface="numpy" and a TorchCircuit for
interface="torch".
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
spec
|
CircuitSpec
|
The circuit to run, usually built with |
required |
observables
|
ObservableLike
|
What to measure. |
None
|
provider
|
ProviderSpec
|
The backend that runs the circuit. It can be a registered name
( |
'numpy'
|
interface
|
Interface
|
How a call is evaluated. With |
'numpy'
|
Example
import numpy as np
from eigenkit import Circuit, Encoding, Variational, all_z
circuit = Circuit(
blocks=[Encoding(in_features=2), Variational(depth=1)],
observables=all_z(2),
)
# The circuit stores no weights, so you pass them at every call.
weights = np.zeros(circuit.spec.n_weights)
values = circuit(weights, np.array([0.1, 0.2]))
# Gradients, without PyTorch.
grad = circuit.jacobian(weights, np.array([0.1, 0.2]))
draw(*, decimals=3)
Return a text drawing of the circuit, over several lines.
The drawing does not depend on the provider: it is built from the
CircuitSpec, not from the compiled backend object. See eigenkit.core.draw
for the details of the layout.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
decimals
|
int
|
The number of significant digits shown for a numeric gate
angle. Default: |
3
|
Returns:
| Type | Description |
|---|---|
str
|
The drawing, as a single string that contains newlines. |
draw_mpl(**kwargs)
Draw the circuit as a matplotlib figure, and return (fig, ax).
Gates are drawn as labelled boxes and controls as filled dots, and each
measured wire (from self.observables) ends with a measurement symbol.
As with draw(), the picture is built from the CircuitSpec and the
observables, not from the compiled backend, so it does not depend on the
provider.
Pass style="eigen" for the brand colours (each gate is coloured by its
kind: rotations, H and block gates, and measurements), or
style="roles" to colour the outline of each gate by its role (encoding,
trainable or fixed). The default is black on white. Each style has a
"-dark" variant (for example "eigen-dark") for dark backgrounds, and
"eigen-universal" is a single image that works on both.
matplotlib is an optional dependency. Install it with eigenkit[viz].
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
**kwargs
|
Any
|
Arguments passed to
|
{}
|
Returns:
| Name | Type | Description |
|---|---|---|
fig_ax |
tuple
|
The matplotlib |
dry_run_info()
Describe the prepared circuit in a dictionary, without submitting it.
It is available only on backends whose CompiledCircuit provides a
dry_run_info method. Currently, these are Braket (on its local simulator
as well as on cloud devices), Qiskit Runtime and IQM. It is useful to check
the size of the circuit, the gate counts after transpilation, the number of
shots and the number of circuits that each call runs, before you submit to
a cloud simulator or a quantum processing unit (QPU). It does not estimate a
price.
jacobian(weights, inputs=None, *, input_grad=False)
Return the gradient of the expectation values with respect to the weights.
It returns d<O>/d(weights), of shape (n_weights,) for a single
observable or (n_observables, n_weights) for a list of observables, like
the output of __call__(). Pass a single 1-D inputs sample. For a batch,
call it once for each row.
The NumPy interface can compute every gradient without PyTorch. This method uses the same sequence of gradient methods as the variational optimisation tools and the PyTorch interface. It uses the backend's own differentiation when the backend has one (the analytic adjoint method of the NumPy simulator, the differentiation of PennyLane, and so on), and otherwise the parameter-shift rule, which works on any backend.
With input_grad=True, it returns (weight_jacobian, input_jacobian),
where input_jacobian is d<O>/d(inputs), with the same leading shape.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
One 1-D sample, of shape |
None
|
input_grad
|
bool
|
If True, also return the jacobian with respect to the
inputs. Default: |
False
|
Returns:
| Name | Type | Description |
|---|---|---|
jacobian |
ndarray | tuple[ndarray, ndarray]
|
The weight
jacobian, or |
Raises:
| Type | Description |
|---|---|
RuntimeError
|
On a hardware backend whose configuration leaves
|
probabilities(weights, inputs=None)
Return the measurement distribution over all 2**n_qubits basis states.
The basis states are ordered with qubit 0 as the most significant bit.
The distribution is used to decode samples. For example, the quantum
approximate optimisation algorithm (QAOA) reads the most probable
bitstrings from the optimised state.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
One 1-D sample. |
None
|
Returns:
| Type | Description |
|---|---|
ndarray
|
The probabilities of all basis states, of shape |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On a backend that has neither a |
resources(**kwargs)
Report the resources that the circuit uses once transpiled for its target.
It reports the native gate counts, the number of two-qubit gates and the two-qubit depth, the physical qubits chosen by the layout, the number of two-qubit gates added by routing (compared with the same circuit on the native gates with all-to-all connectivity), and the success probability predicted by the error rates of the target. Nothing is submitted.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
**kwargs
|
Any
|
Arguments passed to the backend, for example
|
{}
|
Returns:
| Type | Description |
|---|---|
dict
|
A dictionary. See |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On backends that do not transpile for a device,
which includes every simulator. To inspect a device locally, use
Qiskit Runtime or IQM with a fake |
sample(weights, inputs=None)
Return the raw measurement histogram, which maps each bitstring to a count.
It is what a sampling backend measured, before any averaging. These are
the counts behind probabilities(), and it is the only form that stays
usable when the circuit has too many qubits for a dense distribution. In
each bitstring, qubit 0 is the most significant bit, so "100" means
that qubit 0 was measured in state 1.
Only sampling backends can return a histogram, because it needs a finite
number of shots. Exact statevector simulators raise an error instead of
making up a histogram. Use probabilities() with those.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
One 1-D sample. |
None
|
Returns:
| Name | Type | Description |
|---|---|---|
counts |
dict[str, int]
|
The number of shots for each measured bitstring. The counts add up to the number of shots set for the backend. |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On backends that do not sample. This includes every exact simulator, which has no shots to report. |
statevector(weights, inputs=None, initial_state=None)
Return the full complex statevector after the circuit runs.
It is a flat array of length 2**n_qubits, ordered with qubit 0 as the
most significant bit. A 2-D inputs batch returns an array of shape
(B, 2**n_qubits). With initial_state, a normalised flat statevector in
the same order, the evolution starts from that state instead of |0…0⟩.
Reading a state out and passing it back in this way is the basic operation
behind the state carried over in quantum reservoirs and behind amplitude
encoding.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
A 1-D sample, or a 2-D batch. |
None
|
initial_state
|
ndarray | None
|
The state to start the evolution
from, instead of |
None
|
Returns:
| Type | Description |
|---|---|
ndarray
|
The statevector, of shape |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On backends without access to the statevector, which is the case for most quantum processing unit (QPU) and cloud backends. |
submit(weights, inputs=None)
Submit a job without waiting for it, and return a JobHandle.
handle.result() returns the expectation value of each observable.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
One 1-D sample. |
None
|
Returns:
| Name | Type | Description |
|---|---|---|
handle |
JobHandle
|
A handle for the submitted job. |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
If the |
transpiled_circuit(**kwargs)
Return the qiskit.QuantumCircuit that a hardware backend submits.
The circuit is transpiled for the target of the backend. Use it to draw the
circuit (.draw("mpl")) or to inspect it.
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On backends that do not transpile for a device. |
zero_state_probabilities(weights, inputs)
Compute zero_state_probability() for every row of a batch of inputs.
inputs has shape (B, n_inputs), and the result is an array of shape
(B,) of all-zeros probabilities. Backends that provide a batched
zero_state_probabilities (such as the NumPy simulator) compute the whole
batch at once. The other backends call the single-sample method once for
each row. This is what lets QuantumKernel
build a fidelity matrix without a Python loop over pairs of samples.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray
|
A batch, of shape |
required |
Returns:
| Type | Description |
|---|---|
ndarray
|
One all-zeros probability for each row, as an array of shape |
zero_state_probability(weights, inputs=None)
Return the probability of measuring the all-zeros state after the circuit.
It is useful for quantities based on fidelity: quantum kernels built from
inversion circuits, swap tests and the Bures distance. Each backend
computes it in its own way. PennyLane returns qml.probs(...)[0], the
Qiskit and NumPy simulators return the squared amplitude of the all-zeros
basis state, Braket uses its own probability result, and IQM and Qiskit
Runtime estimate it from shots. This method does not go through the
Observable path, because the value is not the expectation value of a
Pauli operator.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
weights
|
ndarray
|
The weight vector, of shape |
required |
inputs
|
ndarray | None
|
One 1-D sample. |
None
|
Returns:
| Type | Description |
|---|---|
float
|
The probability, a float in |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
If the active backend does not provide
|
eigenkit.torch.circuit.TorchCircuit
Bases: Module
A quantum layer that stores trainable weights and runs on any registered backend.
It runs through the PyTorch interface, so that PyTorch can compute the gradients of its output.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
blocks
|
_BlocksOrSpec
|
The circuit. It can be a list of blocks to assemble, a |
required |
observables
|
ObservableLike
|
What to measure. |
None
|
provider
|
ProviderSpec
|
The backend that runs the circuit. It can be a registered name, a
configuration instance, or a provider object. Any backend works. A
backend that computes gradients itself avoids the fallback to the
parameter-shift rule. Default: |
'numpy'
|
init
|
Tensor | None
|
The initial weights, of shape |
None
|
n_qubits
property
The number of qubits of the circuit in spec.
out_features
property
The number of observables, or 1 for a single observable.
provider
property
The backend that this circuit was compiled for.
It is the same as Circuit.provider,
which turns the provider= argument (a registered name, a configuration
or a backend object) into one Provider. The registered name is
provider.name. To run the same circuit on another backend, use
with_provider(), which returns a new instance and leaves this one
unchanged.
spec
property
The circuit that this layer runs.
It is the CircuitSpec assembled from
blocks, or the one that was passed in already assembled.
draw(*, decimals=3)
Return a text drawing of the circuit, over several lines.
The drawing does not depend on the provider: it is built from the
CircuitSpec, so it is the same whatever the active backend is. Print the
returned string directly.
Example
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
decimals
|
int
|
The number of significant digits shown for a numeric gate
angle. Default: |
3
|
Returns:
| Type | Description |
|---|---|
str
|
The drawing, as a single string that contains newlines. |
draw_mpl(**kwargs)
Draw the circuit as a matplotlib figure, and return (fig, ax).
The picture does not depend on the provider, because it is built from the
CircuitSpec and the observables. matplotlib is an optional dependency.
Install it with eigenkit[viz]. The keyword arguments are passed to
draw_mpl().
dry_run_info()
Describe the prepared circuit in a dictionary, without submitting it.
It is useful to check the size of the circuit, the gate counts after
transpilation, the number of shots and the number of circuits that each call
runs, before you submit to a cloud simulator or a quantum processing unit
(QPU). It does not estimate a price. It is available only on the backends that provide it.
Currently, these are Braket (on its local simulator as well as on cloud
devices), Qiskit Runtime and IQM. Other backends raise a
NotImplementedError.
forward(x=None)
Run the layer.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
x
|
Tensor
|
The input batch, of shape |
None
|
Returns:
| Type | Description |
|---|---|
Tensor
|
The output of the layer for that batch. |
reset_parameters()
Draw new circuit weights from the current PyTorch random number generator.
Every nn.Module that PyTorch provides defines this method. The estimators
call model.apply(reset_parameters) after setting the seed, so that
random_state controls the whole initialisation. Without this method,
the estimators would skip the layer: two fits with different values of
random_state would give different classical weights but exactly the
same quantum weights, and a user who restarts with new seeds to escape a
barren plateau would change only the part of the model that is not the
circuit.
sample(x=None)
Return the raw measurement histogram for the current weights and input.
The histogram maps each bitstring to its number of shots. In each
bitstring, qubit 0 is the most significant bit.
It is the second step of the workflow in which you train on a simulator and then run on hardware: you train the layer, and then you read what the device measured. It takes one sample, and its result is not differentiable, because the counts are integers that PyTorch does not record for automatic differentiation.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
x
|
Tensor | None
|
The input features of one sample, as a 1-D
tensor. |
None
|
Returns:
| Name | Type | Description |
|---|---|---|
counts |
dict[str, int]
|
The number of shots for each measured bitstring. |
Raises:
| Type | Description |
|---|---|
NotImplementedError
|
On backends that do not sample. |
ValueError
|
If |
submit(x=None)
Submit a job without waiting for it, and return a JobHandle.
Only the backends that provide submission support it (Braket, Qiskit Runtime and IQM).
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
x
|
Tensor | None
|
One 1-D input sample. |
None
|
Returns:
| Name | Type | Description |
|---|---|---|
handle |
JobHandle
|
A handle for the submitted job. |
with_provider(provider, *, copy_weights=True, init=None)
Return a new TorchCircuit for another provider.
The new circuit has the same spec and the same observables argument as
this instance, and it is compiled for the given provider.
provider accepts the same forms as in __init__(): a registered name
(a str), a configuration object with a make_backend() method (for
example PennyLaneConfig), or a backend instance.
The gradients follow the gradient_method of the new backend. The forward
values should match across simulators up to numerical tolerance, but not
exactly.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
provider
|
ProviderSpec
|
The backend for the new circuit. |
required |
copy_weights
|
bool
|
If True, the new circuit starts from a copy of
|
True
|
init
|
Tensor | None
|
An optional weight tensor of shape |
None
|
Returns:
| Type | Description |
|---|---|
'TorchCircuit'
|
The new |
zero_state_probability(x=None)
Return the probability of measuring the all-zeros state.
It uses the current weights and the given input. It is useful for fidelity kernels and swap tests.
It takes one sample, and its result is not differentiable. The core reads
the amplitude through the backend's access to the state and returns a plain
float, so PyTorch does not record it for automatic differentiation. A
batch raises an error, because a single number cannot hold a batch axis.
For a batch, call this method once for each row, or use
Circuit.zero_state_probabilities.
Parameters:
| Name | Type | Description | Default |
|---|---|---|---|
x
|
Tensor | None
|
The input features of one sample, as a 1-D
tensor. |
None
|
Returns:
| Type | Description |
|---|---|
float
|
The all-zeros probability, a float in |
Raises:
| Type | Description |
|---|---|
ValueError
|
If |