676 lines
17 KiB
Python
676 lines
17 KiB
Python
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"""Pauli operators and states"""
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from sympy.core.add import Add
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from sympy.core.mul import Mul
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from sympy.core.numbers import I
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from sympy.core.power import Pow
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from sympy.core.singleton import S
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from sympy.functions.elementary.exponential import exp
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from sympy.physics.quantum import Operator, Ket, Bra
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from sympy.physics.quantum import ComplexSpace
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from sympy.matrices import Matrix
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from sympy.functions.special.tensor_functions import KroneckerDelta
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__all__ = [
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'SigmaX', 'SigmaY', 'SigmaZ', 'SigmaMinus', 'SigmaPlus', 'SigmaZKet',
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'SigmaZBra', 'qsimplify_pauli'
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]
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class SigmaOpBase(Operator):
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"""Pauli sigma operator, base class"""
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@property
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def name(self):
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return self.args[0]
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@property
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def use_name(self):
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return bool(self.args[0]) is not False
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@classmethod
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def default_args(self):
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return (False,)
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def __new__(cls, *args, **hints):
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return Operator.__new__(cls, *args, **hints)
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def _eval_commutator_BosonOp(self, other, **hints):
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return S.Zero
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class SigmaX(SigmaOpBase):
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"""Pauli sigma x operator
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Parameters
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==========
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name : str
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An optional string that labels the operator. Pauli operators with
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different names commute.
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Examples
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========
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>>> from sympy.physics.quantum import represent
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>>> from sympy.physics.quantum.pauli import SigmaX
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>>> sx = SigmaX()
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>>> sx
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SigmaX()
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>>> represent(sx)
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Matrix([
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[0, 1],
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[1, 0]])
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"""
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def __new__(cls, *args, **hints):
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return SigmaOpBase.__new__(cls, *args, **hints)
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def _eval_commutator_SigmaY(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return 2 * I * SigmaZ(self.name)
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def _eval_commutator_SigmaZ(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return - 2 * I * SigmaY(self.name)
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def _eval_commutator_BosonOp(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaY(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaZ(self, other, **hints):
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return S.Zero
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def _eval_adjoint(self):
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return self
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def _print_contents_latex(self, printer, *args):
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if self.use_name:
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return r'{\sigma_x^{(%s)}}' % str(self.name)
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else:
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return r'{\sigma_x}'
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def _print_contents(self, printer, *args):
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return 'SigmaX()'
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def _eval_power(self, e):
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if e.is_Integer and e.is_positive:
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return SigmaX(self.name).__pow__(int(e) % 2)
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def _represent_default_basis(self, **options):
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format = options.get('format', 'sympy')
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if format == 'sympy':
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return Matrix([[0, 1], [1, 0]])
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else:
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raise NotImplementedError('Representation in format ' +
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format + ' not implemented.')
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class SigmaY(SigmaOpBase):
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"""Pauli sigma y operator
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Parameters
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==========
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name : str
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An optional string that labels the operator. Pauli operators with
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different names commute.
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Examples
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========
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>>> from sympy.physics.quantum import represent
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>>> from sympy.physics.quantum.pauli import SigmaY
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>>> sy = SigmaY()
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>>> sy
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SigmaY()
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>>> represent(sy)
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Matrix([
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[0, -I],
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[I, 0]])
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"""
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def __new__(cls, *args, **hints):
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return SigmaOpBase.__new__(cls, *args)
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def _eval_commutator_SigmaZ(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return 2 * I * SigmaX(self.name)
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def _eval_commutator_SigmaX(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return - 2 * I * SigmaZ(self.name)
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def _eval_anticommutator_SigmaX(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaZ(self, other, **hints):
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return S.Zero
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def _eval_adjoint(self):
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return self
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def _print_contents_latex(self, printer, *args):
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if self.use_name:
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return r'{\sigma_y^{(%s)}}' % str(self.name)
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else:
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return r'{\sigma_y}'
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def _print_contents(self, printer, *args):
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return 'SigmaY()'
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def _eval_power(self, e):
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if e.is_Integer and e.is_positive:
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return SigmaY(self.name).__pow__(int(e) % 2)
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def _represent_default_basis(self, **options):
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format = options.get('format', 'sympy')
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if format == 'sympy':
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return Matrix([[0, -I], [I, 0]])
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else:
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raise NotImplementedError('Representation in format ' +
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format + ' not implemented.')
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class SigmaZ(SigmaOpBase):
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"""Pauli sigma z operator
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Parameters
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==========
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name : str
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An optional string that labels the operator. Pauli operators with
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different names commute.
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Examples
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========
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>>> from sympy.physics.quantum import represent
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>>> from sympy.physics.quantum.pauli import SigmaZ
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>>> sz = SigmaZ()
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>>> sz ** 3
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SigmaZ()
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>>> represent(sz)
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Matrix([
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[1, 0],
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[0, -1]])
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"""
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def __new__(cls, *args, **hints):
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return SigmaOpBase.__new__(cls, *args)
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def _eval_commutator_SigmaX(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return 2 * I * SigmaY(self.name)
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def _eval_commutator_SigmaY(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return - 2 * I * SigmaX(self.name)
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def _eval_anticommutator_SigmaX(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaY(self, other, **hints):
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return S.Zero
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def _eval_adjoint(self):
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return self
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def _print_contents_latex(self, printer, *args):
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if self.use_name:
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return r'{\sigma_z^{(%s)}}' % str(self.name)
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else:
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return r'{\sigma_z}'
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def _print_contents(self, printer, *args):
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return 'SigmaZ()'
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def _eval_power(self, e):
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if e.is_Integer and e.is_positive:
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return SigmaZ(self.name).__pow__(int(e) % 2)
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def _represent_default_basis(self, **options):
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format = options.get('format', 'sympy')
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if format == 'sympy':
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return Matrix([[1, 0], [0, -1]])
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else:
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raise NotImplementedError('Representation in format ' +
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format + ' not implemented.')
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class SigmaMinus(SigmaOpBase):
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"""Pauli sigma minus operator
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Parameters
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==========
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name : str
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An optional string that labels the operator. Pauli operators with
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different names commute.
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Examples
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========
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>>> from sympy.physics.quantum import represent, Dagger
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>>> from sympy.physics.quantum.pauli import SigmaMinus
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>>> sm = SigmaMinus()
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>>> sm
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SigmaMinus()
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>>> Dagger(sm)
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SigmaPlus()
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>>> represent(sm)
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Matrix([
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[0, 0],
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[1, 0]])
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"""
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def __new__(cls, *args, **hints):
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return SigmaOpBase.__new__(cls, *args)
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def _eval_commutator_SigmaX(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return -SigmaZ(self.name)
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def _eval_commutator_SigmaY(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return I * SigmaZ(self.name)
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def _eval_commutator_SigmaZ(self, other, **hints):
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return 2 * self
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def _eval_commutator_SigmaMinus(self, other, **hints):
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return SigmaZ(self.name)
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def _eval_anticommutator_SigmaZ(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaX(self, other, **hints):
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return S.One
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def _eval_anticommutator_SigmaY(self, other, **hints):
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return I * S.NegativeOne
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def _eval_anticommutator_SigmaPlus(self, other, **hints):
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return S.One
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def _eval_adjoint(self):
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return SigmaPlus(self.name)
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def _eval_power(self, e):
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if e.is_Integer and e.is_positive:
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return S.Zero
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def _print_contents_latex(self, printer, *args):
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if self.use_name:
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return r'{\sigma_-^{(%s)}}' % str(self.name)
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else:
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return r'{\sigma_-}'
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def _print_contents(self, printer, *args):
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return 'SigmaMinus()'
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def _represent_default_basis(self, **options):
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format = options.get('format', 'sympy')
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if format == 'sympy':
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return Matrix([[0, 0], [1, 0]])
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else:
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raise NotImplementedError('Representation in format ' +
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format + ' not implemented.')
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class SigmaPlus(SigmaOpBase):
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"""Pauli sigma plus operator
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Parameters
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==========
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name : str
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An optional string that labels the operator. Pauli operators with
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different names commute.
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Examples
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========
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>>> from sympy.physics.quantum import represent, Dagger
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>>> from sympy.physics.quantum.pauli import SigmaPlus
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>>> sp = SigmaPlus()
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>>> sp
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SigmaPlus()
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>>> Dagger(sp)
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SigmaMinus()
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>>> represent(sp)
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Matrix([
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[0, 1],
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[0, 0]])
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"""
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def __new__(cls, *args, **hints):
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return SigmaOpBase.__new__(cls, *args)
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def _eval_commutator_SigmaX(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return SigmaZ(self.name)
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def _eval_commutator_SigmaY(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return I * SigmaZ(self.name)
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def _eval_commutator_SigmaZ(self, other, **hints):
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if self.name != other.name:
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return S.Zero
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else:
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return -2 * self
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def _eval_commutator_SigmaMinus(self, other, **hints):
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return SigmaZ(self.name)
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def _eval_anticommutator_SigmaZ(self, other, **hints):
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return S.Zero
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def _eval_anticommutator_SigmaX(self, other, **hints):
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return S.One
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def _eval_anticommutator_SigmaY(self, other, **hints):
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return I
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def _eval_anticommutator_SigmaMinus(self, other, **hints):
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return S.One
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def _eval_adjoint(self):
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return SigmaMinus(self.name)
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def _eval_mul(self, other):
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return self * other
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def _eval_power(self, e):
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if e.is_Integer and e.is_positive:
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return S.Zero
|
||
|
|
|
||
|
|
def _print_contents_latex(self, printer, *args):
|
||
|
|
if self.use_name:
|
||
|
|
return r'{\sigma_+^{(%s)}}' % str(self.name)
|
||
|
|
else:
|
||
|
|
return r'{\sigma_+}'
|
||
|
|
|
||
|
|
def _print_contents(self, printer, *args):
|
||
|
|
return 'SigmaPlus()'
|
||
|
|
|
||
|
|
def _represent_default_basis(self, **options):
|
||
|
|
format = options.get('format', 'sympy')
|
||
|
|
if format == 'sympy':
|
||
|
|
return Matrix([[0, 1], [0, 0]])
|
||
|
|
else:
|
||
|
|
raise NotImplementedError('Representation in format ' +
|
||
|
|
format + ' not implemented.')
|
||
|
|
|
||
|
|
|
||
|
|
class SigmaZKet(Ket):
|
||
|
|
"""Ket for a two-level system quantum system.
|
||
|
|
|
||
|
|
Parameters
|
||
|
|
==========
|
||
|
|
|
||
|
|
n : Number
|
||
|
|
The state number (0 or 1).
|
||
|
|
|
||
|
|
"""
|
||
|
|
|
||
|
|
def __new__(cls, n):
|
||
|
|
if n not in (0, 1):
|
||
|
|
raise ValueError("n must be 0 or 1")
|
||
|
|
return Ket.__new__(cls, n)
|
||
|
|
|
||
|
|
@property
|
||
|
|
def n(self):
|
||
|
|
return self.label[0]
|
||
|
|
|
||
|
|
@classmethod
|
||
|
|
def dual_class(self):
|
||
|
|
return SigmaZBra
|
||
|
|
|
||
|
|
@classmethod
|
||
|
|
def _eval_hilbert_space(cls, label):
|
||
|
|
return ComplexSpace(2)
|
||
|
|
|
||
|
|
def _eval_innerproduct_SigmaZBra(self, bra, **hints):
|
||
|
|
return KroneckerDelta(self.n, bra.n)
|
||
|
|
|
||
|
|
def _apply_from_right_to_SigmaZ(self, op, **options):
|
||
|
|
if self.n == 0:
|
||
|
|
return self
|
||
|
|
else:
|
||
|
|
return S.NegativeOne * self
|
||
|
|
|
||
|
|
def _apply_from_right_to_SigmaX(self, op, **options):
|
||
|
|
return SigmaZKet(1) if self.n == 0 else SigmaZKet(0)
|
||
|
|
|
||
|
|
def _apply_from_right_to_SigmaY(self, op, **options):
|
||
|
|
return I * SigmaZKet(1) if self.n == 0 else (-I) * SigmaZKet(0)
|
||
|
|
|
||
|
|
def _apply_from_right_to_SigmaMinus(self, op, **options):
|
||
|
|
if self.n == 0:
|
||
|
|
return SigmaZKet(1)
|
||
|
|
else:
|
||
|
|
return S.Zero
|
||
|
|
|
||
|
|
def _apply_from_right_to_SigmaPlus(self, op, **options):
|
||
|
|
if self.n == 0:
|
||
|
|
return S.Zero
|
||
|
|
else:
|
||
|
|
return SigmaZKet(0)
|
||
|
|
|
||
|
|
def _represent_default_basis(self, **options):
|
||
|
|
format = options.get('format', 'sympy')
|
||
|
|
if format == 'sympy':
|
||
|
|
return Matrix([[1], [0]]) if self.n == 0 else Matrix([[0], [1]])
|
||
|
|
else:
|
||
|
|
raise NotImplementedError('Representation in format ' +
|
||
|
|
format + ' not implemented.')
|
||
|
|
|
||
|
|
|
||
|
|
class SigmaZBra(Bra):
|
||
|
|
"""Bra for a two-level quantum system.
|
||
|
|
|
||
|
|
Parameters
|
||
|
|
==========
|
||
|
|
|
||
|
|
n : Number
|
||
|
|
The state number (0 or 1).
|
||
|
|
|
||
|
|
"""
|
||
|
|
|
||
|
|
def __new__(cls, n):
|
||
|
|
if n not in (0, 1):
|
||
|
|
raise ValueError("n must be 0 or 1")
|
||
|
|
return Bra.__new__(cls, n)
|
||
|
|
|
||
|
|
@property
|
||
|
|
def n(self):
|
||
|
|
return self.label[0]
|
||
|
|
|
||
|
|
@classmethod
|
||
|
|
def dual_class(self):
|
||
|
|
return SigmaZKet
|
||
|
|
|
||
|
|
|
||
|
|
def _qsimplify_pauli_product(a, b):
|
||
|
|
"""
|
||
|
|
Internal helper function for simplifying products of Pauli operators.
|
||
|
|
"""
|
||
|
|
if not (isinstance(a, SigmaOpBase) and isinstance(b, SigmaOpBase)):
|
||
|
|
return Mul(a, b)
|
||
|
|
|
||
|
|
if a.name != b.name:
|
||
|
|
# Pauli matrices with different labels commute; sort by name
|
||
|
|
if a.name < b.name:
|
||
|
|
return Mul(a, b)
|
||
|
|
else:
|
||
|
|
return Mul(b, a)
|
||
|
|
|
||
|
|
elif isinstance(a, SigmaX):
|
||
|
|
|
||
|
|
if isinstance(b, SigmaX):
|
||
|
|
return S.One
|
||
|
|
|
||
|
|
if isinstance(b, SigmaY):
|
||
|
|
return I * SigmaZ(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaZ):
|
||
|
|
return - I * SigmaY(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaMinus):
|
||
|
|
return (S.Half + SigmaZ(a.name)/2)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaPlus):
|
||
|
|
return (S.Half - SigmaZ(a.name)/2)
|
||
|
|
|
||
|
|
elif isinstance(a, SigmaY):
|
||
|
|
|
||
|
|
if isinstance(b, SigmaX):
|
||
|
|
return - I * SigmaZ(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaY):
|
||
|
|
return S.One
|
||
|
|
|
||
|
|
if isinstance(b, SigmaZ):
|
||
|
|
return I * SigmaX(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaMinus):
|
||
|
|
return -I * (S.One + SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaPlus):
|
||
|
|
return I * (S.One - SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
elif isinstance(a, SigmaZ):
|
||
|
|
|
||
|
|
if isinstance(b, SigmaX):
|
||
|
|
return I * SigmaY(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaY):
|
||
|
|
return - I * SigmaX(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaZ):
|
||
|
|
return S.One
|
||
|
|
|
||
|
|
if isinstance(b, SigmaMinus):
|
||
|
|
return - SigmaMinus(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaPlus):
|
||
|
|
return SigmaPlus(a.name)
|
||
|
|
|
||
|
|
elif isinstance(a, SigmaMinus):
|
||
|
|
|
||
|
|
if isinstance(b, SigmaX):
|
||
|
|
return (S.One - SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaY):
|
||
|
|
return - I * (S.One - SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaZ):
|
||
|
|
# (SigmaX(a.name) - I * SigmaY(a.name))/2
|
||
|
|
return SigmaMinus(b.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaMinus):
|
||
|
|
return S.Zero
|
||
|
|
|
||
|
|
if isinstance(b, SigmaPlus):
|
||
|
|
return S.Half - SigmaZ(a.name)/2
|
||
|
|
|
||
|
|
elif isinstance(a, SigmaPlus):
|
||
|
|
|
||
|
|
if isinstance(b, SigmaX):
|
||
|
|
return (S.One + SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaY):
|
||
|
|
return I * (S.One + SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaZ):
|
||
|
|
#-(SigmaX(a.name) + I * SigmaY(a.name))/2
|
||
|
|
return -SigmaPlus(a.name)
|
||
|
|
|
||
|
|
if isinstance(b, SigmaMinus):
|
||
|
|
return (S.One + SigmaZ(a.name))/2
|
||
|
|
|
||
|
|
if isinstance(b, SigmaPlus):
|
||
|
|
return S.Zero
|
||
|
|
|
||
|
|
else:
|
||
|
|
return a * b
|
||
|
|
|
||
|
|
|
||
|
|
def qsimplify_pauli(e):
|
||
|
|
"""
|
||
|
|
Simplify an expression that includes products of pauli operators.
|
||
|
|
|
||
|
|
Parameters
|
||
|
|
==========
|
||
|
|
|
||
|
|
e : expression
|
||
|
|
An expression that contains products of Pauli operators that is
|
||
|
|
to be simplified.
|
||
|
|
|
||
|
|
Examples
|
||
|
|
========
|
||
|
|
|
||
|
|
>>> from sympy.physics.quantum.pauli import SigmaX, SigmaY
|
||
|
|
>>> from sympy.physics.quantum.pauli import qsimplify_pauli
|
||
|
|
>>> sx, sy = SigmaX(), SigmaY()
|
||
|
|
>>> sx * sy
|
||
|
|
SigmaX()*SigmaY()
|
||
|
|
>>> qsimplify_pauli(sx * sy)
|
||
|
|
I*SigmaZ()
|
||
|
|
"""
|
||
|
|
if isinstance(e, Operator):
|
||
|
|
return e
|
||
|
|
|
||
|
|
if isinstance(e, (Add, Pow, exp)):
|
||
|
|
t = type(e)
|
||
|
|
return t(*(qsimplify_pauli(arg) for arg in e.args))
|
||
|
|
|
||
|
|
if isinstance(e, Mul):
|
||
|
|
|
||
|
|
c, nc = e.args_cnc()
|
||
|
|
|
||
|
|
nc_s = []
|
||
|
|
while nc:
|
||
|
|
curr = nc.pop(0)
|
||
|
|
|
||
|
|
while (len(nc) and
|
||
|
|
isinstance(curr, SigmaOpBase) and
|
||
|
|
isinstance(nc[0], SigmaOpBase) and
|
||
|
|
curr.name == nc[0].name):
|
||
|
|
|
||
|
|
x = nc.pop(0)
|
||
|
|
y = _qsimplify_pauli_product(curr, x)
|
||
|
|
c1, nc1 = y.args_cnc()
|
||
|
|
curr = Mul(*nc1)
|
||
|
|
c = c + c1
|
||
|
|
|
||
|
|
nc_s.append(curr)
|
||
|
|
|
||
|
|
return Mul(*c) * Mul(*nc_s)
|
||
|
|
|
||
|
|
return e
|