diff --git a/README.md b/README.md
index 4393c79..585a8a9 100644
--- a/README.md
+++ b/README.md
@@ -1,7 +1,7 @@
# monoprop
> because your operators deserve to propagate at escape velocity
-[](https://docs.algorithmiq.fi/monoprop)
+[](https://docs.monoprop.algorithmiq.tech/)
[](https://github.com/Algorithmiq/monoprop/actions/workflows/test.yml)
[](https://codecov.io/gh/Algorithmiq/monoprop)
@@ -18,9 +18,20 @@ the operator across cores and across nodes with MPI.
## Benchmarks
-Check out the comparison of `monoprop` against other open-source Pauli propagation engines in [benches/third_party]!
-
-
+Check out the comparison of `monoprop` against other open-source Pauli propagation engines:
+
+
+
+
+
+
+and against [`MajoranaPropagation.jl`](https://github.com/SparqleSim/MajoranaPropagation.jl):
+
+
+
+
@@ -43,7 +54,9 @@ from monoprop import MajoranaPropagator, ExpGate, Circuit, MajoranaOperator
# Observable m_0 m_1 m_2 m_4, evolved under one Majorana rotation exp(-i θ/2 · M_γ),
# generated by M_γ = i*m_4 m_5.
observable = MajoranaOperator({(0, 1, 2, 4): 1.0}, num_modes=8)
-gate = ExpGate(MajoranaOperator({(4, 5): 1j}, num_modes=8)) # Hermitian generator: weight-2 => imaginary coeff
+gate = ExpGate(
+ MajoranaOperator({(4, 5): 1j}, num_modes=8)
+) # Hermitian generator: weight-2 => imaginary coeff
circuit = Circuit(gates=[gate], parameters=[0.5]) # one angle value per gate
mp = MajoranaPropagator.from_circuit(circuit, observable, cutoff=16)
@@ -56,7 +69,9 @@ Qubit (Pauli) operators are simulated with `PauliPropagator`. Here we back-propa
```python
from monoprop import PauliPropagator, ExpGate, Circuit, PauliOperator, Pauli
-observable = PauliOperator({"ZZ": 1.0}, num_qubits=2) # num_qubits lives on the observable
+observable = PauliOperator(
+ {"ZZ": 1.0}, num_qubits=2
+) # num_qubits lives on the observable
gate = ExpGate(PauliOperator({Pauli("X", 0): 1.0}, num_qubits=2)) # exp(-i θ/2 · X_0)
circuit = Circuit(gates=[gate], parameters=[0.5]) # one angle value per gate