Executing programs on X8 devices¶

In this tutorial, we demonstrate how Strawberry Fields can execute quantum programs on the X8 family of remote photonic devices, via the Xanadu cloud platform. Topics covered include:

• Configuring Strawberry Fields to access the cloud platform,

• Using the RemoteEngine to execute jobs remotely on X8,

• Compiling quantum programs for specific quantum chip architectures,

• Saving and running Blackbird scripts, an assembly language for quantum photonic hardware, and

• Embedding and sampling from bipartite graphs on X8.

Warning

An authentication token is required to access the Xanadu cloud platform. In the following, replace AUTHENTICATION_TOKEN with your personal API token.

If you do not have an authentication token, you can request hardware access via email at sf@xanadu.ai.

Note

What’s in a name?

X8, rather than being a single hardware chip, corresponds to a family of physical devices, with individual names including X8_01.

While X8 is used here to specify any chip in the X8 device class (including X8_01), you may also specify a specific chip ID (such as X8_01) during program compilation and execution.

Before using the RemoteEngine for the first time, we need to configure Strawberry Fields with an authentication token that provides you access to the Xanadu cloud platform. We can do this by using the store_account() function from within Python:

>>> import strawberryfields as sf
>>> sf.store_account("AUTHENTICATION_TOKEN")


This only needs to be executed the first time configuring Strawberry Fields; your account details will be stored to disk, and automatically loaded from now on.

To test that your account credentials correctly authenticate against the cloud platform, you can use the ping() command,

>>> sf.ping()
You have successfully authenticated to the platform!


Note

Strawberry Fields also provides a command line interface for configuring access to the cloud platform and for submitting jobs:

$sf configure --token AUTHENTICATION_TOKEN$ sf --ping
You have successfully authenticated to the platform!


For more details on configuring Strawberry Fields for cloud access, including using the command line interface, see the Photonic hardware quickstart guide.

Device details¶

Below, we will be submitting a job to run on X8.

X8 is an 8-mode chip, with the following restrictions:

At this point, only the parameters r=1, phi=0 are allowed for the two-mode squeezing gates between any pair of signal and idler modes. Eventually, a range of squeezing amplitudes r will be supported.

Executing jobs¶

In this section, we will use Strawberry Fields to submit a simple circuit to the chip.

First, we import NumPy and Strawberry Fields, including the remote engine.

import numpy as np

import strawberryfields as sf
from strawberryfields import ops
from strawberryfields import RemoteEngine


Lets use the random_interferometer() function to generate a random $$4\times 4$$ unitary:

>>> from strawberryfields.utils import random_interferometer
>>> U = random_interferometer(4)
>>> print(U)
array([[-0.13879438-0.47517904j,-0.29303954-0.47264099j,-0.43951987+0.12977568j, -0.03496718-0.48418713j],
[ 0.06065372-0.11292765j, 0.54733962+0.1215551j, -0.50721513+0.56195975j, -0.15923161+0.26606674j],
[ 0.42212573-0.53182417j, -0.2642572 +0.50625182j, 0.19448705+0.28321781j,  0.30281396-0.05582391j],
[ 0.43097587-0.30288974j, 0.07419772-0.21155126j, 0.28335618-0.13633175j, -0.75113453+0.09580304j]])


Next we create an 8-mode quantum program:

prog = sf.Program(8, name="remote_job1")

with prog.context as q:
# Initial squeezed states
# Allowed values are r=1.0 or r=0.0
ops.S2gate(1.0) | (q[0], q[4])
ops.S2gate(1.0) | (q[1], q[5])
ops.S2gate(1.0) | (q[3], q[7])

# Interferometer on the signal modes (0-3)
ops.Interferometer(U) | (q[0], q[1], q[2], q[3])
ops.BSgate(0.543, 0.123) | (q[2], q[0])
ops.Rgate(0.453) | q[1]
ops.MZgate(0.65, -0.54) | (q[2], q[3])

# *Same* interferometer on the idler modes (4-7)
ops.Interferometer(U) | (q[4], q[5], q[6], q[7])
ops.BSgate(0.543, 0.123) | (q[6], q[4])
ops.Rgate(0.453) | q[5]
ops.MZgate(0.65, -0.54) | (q[6], q[7])

ops.MeasureFock() | q


Finally, we create the engine. Similarly to the LocalEngine, the RemoteEngine is in charge of compiling and executing programs. However, it differs in that the program will be executed on remote devices, rather than on local simulators.

Below, we create a remote engine to submit and execute quantum programs on the X8 photonic device.

>>> eng = RemoteEngine("X8")


We can now run the program by calling eng.run, and passing the program to be executed as well as additional runtime options.

>>> results = eng.run(prog, shots=20)
>>> results.samples
array([[0, 0, 1, 0, 1, 0, 1, 0],
[0, 0, 0, 0, 0, 0, 0, 0],
[0, 0, 0, 0, 0, 0, 0, 2],
[0, 0, 0, 0, 0, 1, 0, 0],
[1, 0, 0, 0, 0, 0, 3, 0],
[3, 0, 0, 0, 2, 0, 1, 0],
[0, 1, 0, 0, 0, 1, 1, 0],
[0, 1, 0, 0, 1, 0, 0, 0],
[0, 0, 0, 0, 0, 0, 1, 1],
[0, 0, 0, 0, 0, 0, 0, 0],
[0, 0, 0, 0, 0, 1, 0, 0],
[1, 0, 0, 0, 1, 0, 0, 0],
[0, 0, 0, 0, 0, 0, 1, 0],
[0, 0, 0, 0, 0, 0, 0, 0],
[0, 0, 0, 0, 0, 0, 0, 1],
[0, 0, 0, 0, 0, 0, 0, 1],
[1, 0, 0, 0, 0, 0, 0, 0],
[0, 0, 0, 0, 0, 1, 0, 0],
[0, 0, 1, 1, 0, 2, 1, 2],
[2, 0, 1, 0, 1, 0, 0, 0]])


The samples returned correspond to 20 measurements (or shots) of the 8 mode quantum program above. Some modes have measured zero photons, and others have detected single photons, with a few even detecting 2 or 3.

By taking the average of the returned array along the shots axis, we can estimate the mean photon number of each mode:

>>> np.mean(results.samples, axis=0)
array([0.4, 0.1, 0.15, 0.05, 0.3, 0.3, 0.45, 0.35])


We can also use the Python collections module to convert the samples into counts:

>>> from collections import Counter
>>> bitstrings = [tuple(i) for i in results.samples]
>>> counts = {k:v for k, v in Counter(bitstrings).items()}
>>> counts[(0, 0, 0, 0, 0, 0, 0)]
2


Note

The operation decorator allows you to create your own Strawberry Fields operation. This can make it easier to ensure that the same unitary is always applied to the signal and idler modes.

from strawberryfields.utils import operation

@operation(4)
def unitary(q):
ops.Interferometer(U) | q
ops.BSgate(0.543, 0.123) | (q[2], q[0])
ops.Rgate(0.453) | q[1]
ops.MZgate(0.65, -0.54) | (q[2], q[3])

prog = sf.Program(8)

with prog.context as q:
ops.S2gate(1.0) | (q[0], q[4])
ops.S2gate(1.0) | (q[1], q[5])
ops.S2gate(1.0) | (q[3], q[7])

unitary() | q[:4]
unitary() | q[4:]

ops.MeasureFock() | q


Refer to the operation documentation for more details.

Job management¶

Above, when we called eng.run(), we had to wait for the remote device to execute the program and the result to be returned before we could continue executing code. That is, eng.run() is a blocking method.

Sometimes, however, it is useful to submit the program and continue performing computation locally, every now and again checking to see if the job is complete and the results are ready. This is possible with the non-blocking eng.run_async() method:

>>> job = engine.run_async(program, shots=100)


Unlike eng.run(), it returns a Job instance, which allows us to check the status of our submitted job:

>>> job.id
>>> job.status
"queued"


When the job result is ready, it is available via the result property. If the job result is not yet available, however, an InvalidJobOperationError will be raised:

>>> job.result
InvalidJobOperationError


To check when the results are ready, the job can be refreshed, and the status checked:

>>> job.refresh()
>>> job.status
"complete"
>>> result = job.result
>>> result.samples.shape
(100, 8)


Finally, an incomplete job can be cancelled by calling job.cancel().

Hardware compilation¶

When creating a quantum program to run on hardware, Strawberry Fields can compile any collection of the following gates into a multi-mode unitary:

Furthermore, several automatic decompositions are supported:

• You can use the Interferometer command to directly pass a unitary matrix to be decomposed and compiled to match the device architecture. This performs a rectangular decomposition using Mach-Zehnder interferometers.

• You can use BipartiteGraphEmbed to embed a bipartite graph on the photonic device.

Warning

Decomposed squeezing values depend on the graph structure, so only bipartite graphs that result in equal squeezing on all modes can be executed on X8 chips.

Before sending the program to the cloud platform to be executed, however, Strawberry Fields must compile the program to match the physical architecture or layout of the photonic chip, in this case X8. This happens implicitly when using the remote engine, however we can use the compile() method to explicitly compile the program for a specific chip.

For example, lets compile the program we created in the previous section:

>>> prog_compiled = prog.compile("X8")
>>> prog_compiled.print()
S2gate(1, 0) | (q[0], q[4])
S2gate(1, 0) | (q[3], q[7])
S2gate(1, 0) | (q[2], q[6])
MZgate(1.573, 4.368) | (q[2], q[3])
MZgate(1.573, 4.368) | (q[6], q[7])
S2gate(1, 0) | (q[1], q[5])
MZgate(1.228, 5.006) | (q[0], q[1])
MZgate(4.414, 3.859) | (q[1], q[2])
MZgate(2.98, 3.316) | (q[2], q[3])
Rgate(-0.7501) | (q[3])
MZgate(5.397, 5.494) | (q[0], q[1])
MZgate(5.152, 4.891) | (q[1], q[2])
Rgate(2.544) | (q[2])
MZgate(1.228, 5.006) | (q[4], q[5])
MZgate(4.414, 3.859) | (q[5], q[6])
MZgate(2.98, 3.316) | (q[6], q[7])
Rgate(-0.7501) | (q[7])
MZgate(5.397, 5.494) | (q[4], q[5])
MZgate(5.152, 4.891) | (q[5], q[6])
Rgate(2.544) | (q[6])
Rgate(-1.173) | (q[1])
Rgate(1.902) | (q[4])
Rgate(1.902) | (q[0])
Rgate(-1.173) | (q[5])
MeasureFock | (q[0], q[1], q[2], q[3], q[4], q[5], q[6], q[7])


While equivalent to the uncompiled program, we can now see the low-level hardware operations that are applied on the physical chip.

Working with Blackbird scripts¶

When submitting quantum programs to be executed remotely, they are communicated to the cloud platform using Blackbird—a quantum photonic assembly language. Strawberry Fields also supports exporting programs directly as Blackbird scripts (an xbb file); Blackbird scripts can then be submitted to be executed via the Strawberry Fields command line interface.

For example, lets consider a Blackbird script examples/example_job_X8.xbb representing the same quantum program we constructed above:

name remote_job1
version 1.0
target X8 (shots = 20)

complex array U[4, 4] =
-0.13879438-0.47517904j, -0.29303954-0.47264099j, -0.43951987+0.12977568j, -0.03496718-0.48418713j
0.06065372-0.11292765j, 0.54733962+0.1215551j, -0.50721513+0.56195975j, -0.15923161+0.26606674j
0.42212573-0.53182417j, -0.2642572+0.50625182j, 0.19448705+0.28321781j, 0.30281396-0.05582391j
0.43097587-0.30288974j, 0.07419772-0.21155126j, 0.28335618-0.13633175j, -0.75113453+0.09580304j

# Initial states are two-mode squeezed states
S2gate(1.0, 0.0) | [0, 4]
S2gate(1.0, 0.0) | [1, 5]
S2gate(1.0, 0.0) | [3, 7]

# Apply the unitary matrix above to
# the first pair of modes, as well
# as a beamsplitter
Interferometer(U) | [0, 1, 2, 3]
BSgate(0.543, 0.123) | [2, 0]
Rgate(0.453) | 1
MZgate(0.65, -0.54) | [2, 3]

# Duplicate the above unitary for
# the second pair of modes
Interferometer(U) | [4, 5, 6, 7]
BSgate(0.543, 0.123) | [6, 4]
Rgate(0.453) | 5
MZgate(0.65, -0.54) | [6, 7]

# Perform a PNR measurement in the Fock basis
MeasureFock() | [0, 1, 2, 3, 4, 5, 6, 7]


The above Blackbird script can be remotely executed using the command line,

\$ sf run program1.xbb --output out.txt


After executing the above command, the result will be stored in out.txt in the current working directory. You can also omit the --output parameter to print the result to the screen.

Note

Saved Blackbird scripts can be imported as Strawberry Fields programs using the load() function:

>>> prog = load("test.xbb")


Strawberry Fields programs can also be exported as Blackbird scripts using save():

>>> sf.save("program1.xbb", prog)


Embedding bipartite graphs¶

The X8 device class supports embedding bipartite graphs, i.e., those with adjacency matrices

$\begin{split}A = \begin{bmatrix}0 & B\\ B^T & 0\end{bmatrix}\end{split}$

where $$B$$ represents the edges between the two sets of vertices in the graph. However, the devices are currently restricted to bipartite graphs with equally sized partitions, such that the singular values form the set $$\{0, d\}$$ for some real value $$d$$.

Here, we will consider a complete bipartite graph, since the singular values are of the form $$\{0, d\}$$.

B = np.ones([4, 4])
A = np.block([[0*B, B], [B.T, 0*B]])

prog = sf.Program(8)

# the following mean photon number per mode
# quantity is set to ensure that the singular values
# are scaled such that all Sgates have squeezing value r=1
m = 0.345274461385554870545

with prog.context as q:
ops.BipartiteGraphEmbed(A, mean_photon_per_mode=m) | q
ops.MeasureFock() | q

>>> prog.compile("X8").print()
S2gate(1, 0) | (q[0], q[4])
S2gate(0, 0) | (q[3], q[7])
S2gate(0, 0) | (q[2], q[6])
MZgate(3.598, 5.444) | (q[2], q[3])
MZgate(3.598, 5.444) | (q[6], q[7])
S2gate(0, 0) | (q[1], q[5])
MZgate(0, 5.236) | (q[0], q[1])
MZgate(4.886, 5.496) | (q[1], q[2])
MZgate(0.7106, 4.492) | (q[2], q[3])
Rgate(0.9284) | (q[3])
MZgate(2.922, 3.142) | (q[0], q[1])
MZgate(4.528, 3.734) | (q[1], q[2])
Rgate(-2.51) | (q[2])
MZgate(0, 5.236) | (q[4], q[5])
MZgate(4.886, 5.496) | (q[5], q[6])
MZgate(0.7106, 4.492) | (q[6], q[7])
Rgate(0.9284) | (q[7])
MZgate(2.922, 3.142) | (q[4], q[5])
MZgate(4.528, 3.734) | (q[5], q[6])
Rgate(-2.51) | (q[6])
Rgate(-2.51) | (q[1])
Rgate(-0.8273) | (q[4])
Rgate(-0.8273) | (q[0])
Rgate(-2.51) | (q[5])
MeasureFock | (q[0], q[1], q[2], q[3], q[4], q[5], q[6], q[7])


If the bipartite graph to be embedded does not satisfy the aforementioned restriction on the singular values, an error message will be raised on compilation:

>>> B = np.array([[0, 1, 0, 1], [1, 0, 1, 0], [0, 1, 1, 1], [1, 0, 1, 0]])
>>> A = np.block([[np.zeros_like(B), B], [B.T, np.zeros_like(B)]])
>>> prog = sf.Program(8)
>>> with prog.context as q:
...     ops.BipartiteGraphEmbed(A, mean_photon_per_mode=1) | q
...     ops.MeasureFock() | q
CircuitError: Incorrect squeezing value(s) (r, phi)={(1.336, 0.0), (0.177, 0.0), (0.818, 0.0)}.
Allowed squeezing value(s) are (r, phi)={(1.0, 0.0), (0.0, 0.0)}.