docs

mrmustard/lab_dev/circuit_components.py

@@ -526,16 +526,15 @@ def to_bargmann(self) -> CircuitComponent:
         .. code-block::
 
             >>> from mrmustard.lab_dev import Dgate
-            >>> from mrmustard.physics.representations import Bargmann
+            >>> from mrmustard.physics.ansatz import PolyExpAnsatz
 
             >>> d = Dgate([1], x=0.1, y=0.1)
             >>> d_fock = d.to_fock(shape=3)
             >>> d_bargmann = d_fock.to_bargmann()
 
-
             >>> assert d_bargmann.name == d.name
             >>> assert d_bargmann.wires == d.wires
-            >>> assert isinstance(d_bargmann.representation, Bargmann)
+            >>> assert isinstance(d_bargmann.ansatz, PolyExpAnsatz)
         """
         if isinstance(self.ansatz, PolyExpAnsatz):
             return self

mrmustard/lab_dev/states/base.py

@@ -184,7 +184,7 @@ def from_bargmann(
 
         .. code-block::
 
-            >>> from mrmustard.physics.representations import Bargmann
+            >>> from mrmustard.physics.ansatz import PolyExpAnsatz
             >>> from mrmustard.physics.triples import coherent_state_Abc
             >>> from mrmustard.lab_dev.states.base import Ket
 
@@ -193,7 +193,7 @@ def from_bargmann(
 
             >>> coh = Ket.from_bargmann(modes, triple)
             >>> assert coh.modes == modes
-            >>> assert coh.representation == Bargmann(*triple)
+            >>> assert coh.ansatz == PolyExpAnsatz(*triple)
             >>> assert isinstance(coh, Ket)
 
         Args:

mrmustard/physics/ansatz/polyexp_ansatz.py

@@ -72,14 +72,14 @@ class PolyExpAnsatz(Ansatz):
 
     .. code-block ::
 
-        >>> from mrmustard.physics.representations import Bargmann
+        >>> from mrmustard.physics.representations import PolyExpAnsatz
         >>> from mrmustard.physics.triples import displacement_gate_Abc, vacuum_state_Abc
 
         >>> # bargmann representation of one-mode vacuum
-        >>> rep_vac = Bargmann(*vacuum_state_Abc(1))
+        >>> rep_vac = PolyExpAnsatz(*vacuum_state_Abc(1))
 
         >>> # bargmann representation of one-mode dgate with gamma=1+0j
-        >>> rep_dgate = Bargmann(*displacement_gate_Abc(1))
+        >>> rep_dgate = PolyExpAnsatz(*displacement_gate_Abc(1))
 
     The inner product is defined as the contraction of two Bargmann objects across marked indices.
     Indices are marked using ``__getitem__``. Once the indices are marked for contraction, they are