def build_hamiltonian(self):
hilbertspc = self.hilbertspace_initialize()
[transmon1, transmon2, resonator] = hilbertspc
hres = hilbertspc.diag_hamiltonian(resonator)
h1 = hilbertspc.diag_hamiltonian(transmon1)
h2 = hilbertspc.diag_hamiltonian(transmon2)
g1 = 0.1 # coupling resonator-transmon1 (without charge matrix elements)
g2 = 0.2 # coupling resonator-transmon2 (without charge matrix elements)
dim1 = transmon1.truncated_dim
dim2 = transmon2.truncated_dim
_, evecs1 = transmon1.eigensys(dim1)
_, evecs2 = transmon2.eigensys(dim2)
gmat1 = g1 * get_matrixelement_table(
transmon1.n_operator(), evecs1) # coupling constants for transmon1
gmat2 = g2 * get_matrixelement_table(transmon2.n_operator(),
evecs2) # and for transmon2
hbd = hilbertspc.hubbard_operator
a = hilbertspc.annihilate(resonator)
hamiltonian0 = h1 + h2 + hres
vcpb1 = sum([
gmat1[j][k] * hbd(j, k, transmon1) for j in range(dim1)
for k in range(dim1)
])
vcpb2 = sum([
gmat2[j][k] * hbd(j, k, transmon2) for j in range(dim2)
for k in range(dim2)
])
hamiltonian1 = (vcpb1 + vcpb2) * (a + a.dag())
return hamiltonian0 + hamiltonian1
def matrixelement_table(self,
operator: str,
evecs: ndarray = None,
evals_count: int = 6,
filename: str = None,
return_datastore: bool = False) -> ndarray:
"""Returns table of matrix elements for `operator` with respect to the eigenstates of the qubit.
The operator is given as a string matching a class method returning an operator matrix.
E.g., for an instance `trm` of Transmon, the matrix element table for the charge operator is given by
`trm.op_matrixelement_table('n_operator')`.
When `esys` is set to `None`, the eigensystem is calculated on-the-fly.
Parameters
----------
operator:
name of class method in string form, returning operator matrix in qubit-internal basis.
evecs:
if not provided, then the necessary eigenstates are calculated on the fly
evals_count:
number of desired matrix elements, starting with ground state (default value = 6)
filename:
output file name
return_datastore:
if set to true, the returned data is provided as a DataStore object (default value = False)
"""
if evecs is None:
_, evecs = self.eigensys(evals_count=evals_count)
operator_matrix = getattr(self, operator)()
table = get_matrixelement_table(operator_matrix, evecs)
if filename or return_datastore:
data_store = DataStore(system_params=self.get_initdata(),
matrixelem_table=table)
if filename:
data_store.filewrite(filename)
return data_store if return_datastore else table
def _zeropi_operator_in_product_basis(self,
zeropi_operator,
zeropi_evecs=None):
"""Helper method that converts a zeropi operator into one in the product basis.
Returns
-------
scipy.sparse.csc_matrix
operator written in the product basis
"""
zeropi_dim = self.zeropi_cutoff
zeta_dim = self.zeta_cutoff
if zeropi_evecs is None:
_, zeropi_evecs = self._zeropi.eigensys(evals_count=zeropi_dim)
op_eigen_basis = sparse.dia_matrix(
(zeropi_dim, zeropi_dim),
dtype=np.complex_) # is this guaranteed to be zero?
op_zeropi = get_matrixelement_table(zeropi_operator, zeropi_evecs)
for n in range(zeropi_dim):
for m in range(zeropi_dim):
op_eigen_basis += op_zeropi[n, m] * op.hubbard_sparse(
n, m, zeropi_dim)
return sparse.kron(op_eigen_basis,
sparse.identity(zeta_dim,
format='csc',
dtype=np.complex_),
format='csc')
def g_phi_coupling_matrix(self, zeropi_states: ndarray) -> ndarray:
"""Returns a matrix of coupling strengths g^\\phi_{ll'} [cmp. Dempster et al., Eq. (18)], using the states
from the list `zeropi_states`. Most commonly, `zeropi_states` will contain eigenvectors of the
`DisorderedZeroPi` type.
"""
prefactor = self.EL * (self.dEL / 2.0) * (8.0 * self.EC / self.EL) ** 0.25
return prefactor * spec_utils.get_matrixelement_table(self._zeropi.phi_operator(), zeropi_states)
def g_theta_coupling_matrix(self, zeropi_states):
"""Returns a matrix of coupling strengths i*g^\\theta_{ll'} [cmp. Dempster et al., Eq. (17)], using the states
from the list 'zeropi_states'.
"""
prefactor = 1j * self.ECS * (self.dC / 2.0) * (32.0 * self.EL /
self.EC)**0.25
return prefactor * get_matrixelement_table(
self._zeropi.n_theta_operator(), zeropi_states)
def manual_hamiltonian(self, esys1=None, esys2=None):
hilbertspc = self.hilbertspace_initialize()
[fluxonium, zpifull] = hilbertspc
g1 = 0.1
dim1 = fluxonium.truncated_dim
if esys1 is None:
evals1, evecs1 = fluxonium.eigensys(dim1)
else:
evals1, evecs1 = esys1
dim2 = zpifull.truncated_dim
if esys2 is None:
evals2, evecs2 = zpifull.eigensys(dim1)
else:
evals2, evecs2 = esys2
h1 = hilbertspc.diag_hamiltonian(fluxonium, evals=evals1)
h2 = hilbertspc.diag_hamiltonian(zpifull, evals=evals2)
nmat1 = get_matrixelement_table(
fluxonium.n_operator(), evecs1
) # coupling constants for fluxonium
nmat2 = get_matrixelement_table(
zpifull.n_theta_operator(), evecs2
) # coupling constants for zeropi
hbd = hilbertspc.hubbard_operator
vfl = sum(
[
nmat1[j][k] * hbd(j, k, fluxonium)
for j in range(dim1)
for k in range(dim1)
]
)
vzp = sum(
[nmat2[j][k] * hbd(j, k, zpifull) for j in range(dim2) for k in range(dim2)]
)
bare_hamiltonian = h1 + h2
interaction_hamiltonian = g1 * vfl * vzp
return bare_hamiltonian, interaction_hamiltonian
def matrixelement_table(self, operator: str) -> ndarray:
"""Returns table of matrix elements for `operator` with respect to the
eigenstates of the qubit. The operator is given as a string matching a class
method returning an operator matrix.
Parameters
----------
operator:
name of class method in string form, returning operator matrix in
qubit-internal basis.
"""
_, evecs = self.eigensys()
operator_matrix = getattr(self, operator)()
table = get_matrixelement_table(operator_matrix, evecs)
return table
def hamiltonian(self, flux):
hilbertspc = self.hilbertspace_initialize()
[transmon1, transmon2, resonator] = hilbertspc
hres = hilbertspc.diag_hamiltonian(resonator)
# Get diagonalized transmon1 Hamiltonian as full-system operator via tensor product with identities.
g1 = 0.1 # coupling resonator-transmon1 (without charge matrix elements)
g2 = 0.2 # coupling resonator-transmon2 (without charge matrix elements)
dim1 = transmon1.truncated_dim
dim2 = transmon2.truncated_dim
_, evecs1 = transmon1.eigensys(dim1)
_, evecs2 = transmon2.eigensys(dim2)
gmat1 = g1 * get_matrixelement_table(
transmon1.n_operator(), evecs1) # coupling constants for transmon1
gmat2 = g2 * get_matrixelement_table(transmon2.n_operator(),
evecs2) # and for transmon2
hbd = hilbertspc.hubbard_operator
a = hilbertspc.annihilate(resonator)
vcpb1 = sum([
gmat1[j][k] * hbd(j, k, transmon1) for j in range(dim1)
for k in range(dim1)
])
vcpb2 = sum([
gmat2[j][k] * hbd(j, k, transmon2) for j in range(dim2)
for k in range(dim2)
])
transmon1.EJ = 40.0 * np.cos(np.pi * flux)
h1 = hilbertspc.diag_hamiltonian(transmon1)
h2 = hilbertspc.diag_hamiltonian(transmon2)
return h1 + h2 + hres + (vcpb1 + vcpb2) * (a + a.dag())
def qubit_matrixelement(sweep, param_index, qubit_subsys, qubit_operator):
"""
For given ParameterSweep and parameter_index, calculate the matrix elements for the provided qubit operator.
Parameters
----------
sweep: ParameterSweep
param_index: int
qubit_subsys: QuantumSystem
qubit_operator: ndarray
operator within the qubit subspace
Returns
-------
ndarray
"""
bare_evecs = sweep.lookup.bare_eigenstates(param_index, qubit_subsys)
return spectrum_utils.get_matrixelement_table(qubit_operator, bare_evecs)
def identity_wrap(self, operator, subsystem, op_in_eigenbasis=False, evecs=None):
"""Wrap given operator in subspace `subsystem` in identity operators to form full Hilbert-space operator.
Parameters
----------
operator: ndarray or qutip.Qobj or str
operator acting in Hilbert space of `subsystem`; if str, then this should be an operator name in
the subsystem, typically not in eigenbasis
subsystem: object derived from QuantumSystem
subsystem where diagonal operator is defined
op_in_eigenbasis: bool
whether `operator` is given in the `subsystem` eigenbasis; otherwise, the internal QuantumSystem basis is
assumed
evecs: ndarray, optional
internal QuantumSystem eigenstates, used to convert `operator` into eigenbasis
Returns
-------
qutip.Qobj operator
"""
dim = subsystem.truncated_dim
if isinstance(operator, np.ndarray):
if op_in_eigenbasis is False:
if evecs is None:
_, evecs = subsystem.eigensys(evals_count=subsystem.truncated_dim)
operator_matrixelements = get_matrixelement_table(operator, evecs)
subsys_operator = qt.Qobj(inpt=operator_matrixelements)
else:
subsys_operator = qt.Qobj(inpt=operator[:dim, :dim])
elif isinstance(operator, str):
if evecs is None:
_, evecs = subsystem.eigensys(evals_count=subsystem.truncated_dim)
operator_matrixelements = subsystem.matrixelement_table(operator, evecs=evecs)
subsys_operator = qt.Qobj(inpt=operator_matrixelements)
elif isinstance(operator, qt.Qobj):
subsys_operator = operator
else:
raise TypeError('Unsupported operator type: ', type(operator))
operator_identitywrap_list = [qt.operators.qeye(the_subsys.truncated_dim) for the_subsys in self]
subsystem_index = self.get_subsys_index(subsystem)
operator_identitywrap_list[subsystem_index] = subsys_operator
return qt.tensor(operator_identitywrap_list)
def qubit_matrixelement(
sweep: "ParameterSweep",
param_index: int,
qubit_subsys: "QubitBaseClass",
qubit_operator: ndarray,
) -> ndarray:
"""
For given ParameterSweep and parameter_index, calculate the matrix elements for the provided qubit operator.
Parameters
----------
sweep:
param_index:
qubit_subsys:
qubit_operator:
operator within the qubit subspace
"""
bare_evecs = sweep.lookup.bare_eigenstates(qubit_subsys, param_index=param_index)
return spec_utils.get_matrixelement_table(qubit_operator, bare_evecs)
def matrixelement_table(self,
operator,
evecs=None,
evals_count=6,
filename=None):
"""Returns table of matrix elements for `operator` with respect to the eigenstates of the qubit.
The operator is given as a string matching a class method returning an operator matrix.
E.g., for an instance `trm` of Transmon, the matrix element table for the charge operator is given by
`trm.op_matrixelement_table('n_operator')`.
When `esys` is set to `None`, the eigensystem is calculated on-the-fly.
Parameters
----------
operator: str
name of class method in string form, returning operator matrix in qubit-internal basis.
evecs: ndarray, optional
if not provided, then the necesssary eigenstates are calculated on the fly
evals_count: int, optional
number of desired matrix elements, starting with ground state (default value = 6)
filename: str, optional
output file name
Returns
-------
ndarray
"""
if evecs is None:
_, evecs = self.eigensys(evals_count=evals_count)
operator_matrix = getattr(self, operator)()
table = get_matrixelement_table(operator_matrix, evecs)
if filename:
specdata = SpectrumData(energy_table=np.empty(0),
system_params=self._get_metadata_dict(),
param_name='const_parameters',
param_vals=np.empty(0),
matrixelem_table=table)
specdata.filewrite(filename)
return table
