| """1D quantum particle in a box.""" |
|
|
| from sympy.core.numbers import pi |
| from sympy.core.singleton import S |
| from sympy.core.symbol import Symbol |
| from sympy.functions.elementary.miscellaneous import sqrt |
| from sympy.functions.elementary.trigonometric import sin |
| from sympy.sets.sets import Interval |
|
|
| from sympy.physics.quantum.operator import HermitianOperator |
| from sympy.physics.quantum.state import Ket, Bra |
| from sympy.physics.quantum.constants import hbar |
| from sympy.functions.special.tensor_functions import KroneckerDelta |
| from sympy.physics.quantum.hilbert import L2 |
|
|
| m = Symbol('m') |
| L = Symbol('L') |
|
|
|
|
| __all__ = [ |
| 'PIABHamiltonian', |
| 'PIABKet', |
| 'PIABBra' |
| ] |
|
|
|
|
| class PIABHamiltonian(HermitianOperator): |
| """Particle in a box Hamiltonian operator.""" |
|
|
| @classmethod |
| def _eval_hilbert_space(cls, label): |
| return L2(Interval(S.NegativeInfinity, S.Infinity)) |
|
|
| def _apply_operator_PIABKet(self, ket, **options): |
| n = ket.label[0] |
| return (n**2*pi**2*hbar**2)/(2*m*L**2)*ket |
|
|
|
|
| class PIABKet(Ket): |
| """Particle in a box eigenket.""" |
|
|
| @classmethod |
| def _eval_hilbert_space(cls, args): |
| return L2(Interval(S.NegativeInfinity, S.Infinity)) |
|
|
| @classmethod |
| def dual_class(self): |
| return PIABBra |
|
|
| def _represent_default_basis(self, **options): |
| return self._represent_XOp(None, **options) |
|
|
| def _represent_XOp(self, basis, **options): |
| x = Symbol('x') |
| n = Symbol('n') |
| subs_info = options.get('subs', {}) |
| return sqrt(2/L)*sin(n*pi*x/L).subs(subs_info) |
|
|
| def _eval_innerproduct_PIABBra(self, bra): |
| return KroneckerDelta(bra.label[0], self.label[0]) |
|
|
|
|
| class PIABBra(Bra): |
| """Particle in a box eigenbra.""" |
|
|
| @classmethod |
| def _eval_hilbert_space(cls, label): |
| return L2(Interval(S.NegativeInfinity, S.Infinity)) |
|
|
| @classmethod |
| def dual_class(self): |
| return PIABKet |
|
|