Magdagdag ng mga fermionic transition sa pool ng mga configuration
Dito ipinapakita namin ang mga functionality para palawakin ang pool ng mga electronic configuration na nakukuha mula sa aksyon ng mga transition operator sa bawat electronic configuration.
Ipinapakita namin kung paano magdagdag ng single-electron hop ng uri:
para sa at , at para sa lahat ng sa batch ng mga electronic configuration. Sisimulan natin sa pag-generate ng batch ng mga random na electronic configuration:
# Added by doQumentation — installs the packages this notebook needs if they are missing
import importlib.util
_needed = {"numpy": "numpy", "qiskit_addon_sqd": "qiskit-addon-sqd"}
_missing = [pip for module, pip in _needed.items()
if importlib.util.find_spec(module) is None]
# One at a time, so a package that fails to install does not block the others
for _pip in _missing:
%pip install -q {_pip}
if not _missing:
print("\u2713 All required packages are installed")
import numpy as np
n_qubits = 8
n_orb = n_qubits // 2
rand_seed = 22
np.random.seed(rand_seed)
# Generate some random bitstrings for testing
def random_bitstrings(n_samples, n_qubits):
return (
np.round(np.random.rand(n_samples, n_qubits))
.astype("int")
.astype("bool")
)
bitstring_matrix = random_bitstrings(100, n_qubits)
Ang mga excitation operator ay tinutukoy sa loob ng isang numpy array na ang haba ay pareho sa bilang ng mga fermionic node (o qubit). Ang bawat elemento ng array ay dapat isang string na maaaring magkaroon ng mga halagang:
-
'I': Identity -
'+': Operator ng paglikha -
'-': Operator ng pagpuksa
Ginagawa namin ang lahat ng posibleng single-electron transition (sa pagitan ng parehong spin species).
transitions_single = np.array(
[
["I" for i in range(2 * n_orb)]
for j in range(4 * (n_orb**2 - n_orb) // 2 + 1)
]
)
count = 1
for i in range(n_orb):
for j in range(i + 1, n_orb):
# spin up
transitions_single[count, i] = "+"
transitions_single[count, j] = "-"
count += 1
transitions_single[count, i] = "-"
transitions_single[count, j] = "+"
count += 1
# spin down
transitions_single[count, i + n_orb] = "+"
transitions_single[count, j + n_orb] = "-"
count += 1
transitions_single[count, i + n_orb] = "-"
transitions_single[count, j + n_orb] = "+"
count += 1
print(transitions_single)
[['I' 'I' 'I' 'I' 'I' 'I' 'I' 'I']
['+' '-' 'I' 'I' 'I' 'I' 'I' 'I']
['-' '+' 'I' 'I' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' '+' '-' 'I' 'I']
['I' 'I' 'I' 'I' '-' '+' 'I' 'I']
['+' 'I' '-' 'I' 'I' 'I' 'I' 'I']
['-' 'I' '+' 'I' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' '+' 'I' '-' 'I']
['I' 'I' 'I' 'I' '-' 'I' '+' 'I']
['+' 'I' 'I' '-' 'I' 'I' 'I' 'I']
['-' 'I' 'I' '+' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' '+' 'I' 'I' '-']
['I' 'I' 'I' 'I' '-' 'I' 'I' '+']
['I' '+' '-' 'I' 'I' 'I' 'I' 'I']
['I' '-' '+' 'I' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' 'I' '+' '-' 'I']
['I' 'I' 'I' 'I' 'I' '-' '+' 'I']
['I' '+' 'I' '-' 'I' 'I' 'I' 'I']
['I' '-' 'I' '+' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' 'I' '+' 'I' '-']
['I' 'I' 'I' 'I' 'I' '-' 'I' '+']
['I' 'I' '+' '-' 'I' 'I' 'I' 'I']
['I' 'I' '-' '+' 'I' 'I' 'I' 'I']
['I' 'I' 'I' 'I' 'I' 'I' '+' '-']
['I' 'I' 'I' 'I' 'I' 'I' '-' '+']]
Ngayon, ina-apply natin ang mga transition operator sa mga configuration sa bitstring_matrix:
from qiskit_addon_sqd.fermion import enlarge_batch_from_transitions
bitstring_matrix_aug = enlarge_batch_from_transitions(
bitstring_matrix, transitions_single
)
print(bitstring_matrix_aug.shape)
print(bitstring_matrix_aug)
(723, 8)
[[False False False ... False False True]
[False True False ... True False False]
[ True True True ... True False True]
...
[ True False True ... False False True]
[ True True True ... True False True]
[False False False ... False False True]]