Docstrings, array dtypes, fix _sswk "constructor"
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@ -947,13 +947,16 @@ cdef class ScatteringSystem:
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return retdict
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return retdict
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@boundscheck(False)
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@boundscheck(False)
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def scattered_E(self, cdouble wavenumber, scatcoeffvector_full, evalpos, bint alt=False, btyp=BesselType.HANKEL_PLUS):
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def scattered_E(self, cdouble wavenumber, scatcoeffvector_full, evalpos, btyp=BesselType.HANKEL_PLUS, bint alt=False):
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# TODO DOC, periodic systems
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if self.lattice_dimension != 0: # TODO enable also periodic systems
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raise NotImplementedError("For periodic system, use _ScatteringSystemAtOmegaK.scattered_E")
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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evalpos = np.array(evalpos, dtype=float, copy=False)
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evalpos = np.array(evalpos, dtype=float, copy=False)
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if evalpos.shape[-1] != 3:
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if evalpos.shape[-1] != 3:
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raise ValueError("Last dimension of evalpos has to be 3")
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raise ValueError("Last dimension of evalpos has to be 3")
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, copy=False)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, copy=False, dtype=complex)
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cdef cdouble[::1] scv_view = scv
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cdef cdouble[::1] scv_view = scv
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef ccart3_t res
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cdef ccart3_t res
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@ -1003,6 +1006,8 @@ def empty_lattice_modes_xy(EpsMu epsmu, reciprocal_basis, wavevector, double max
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cdef class _ScatteringSystemAtOmegaK:
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cdef class _ScatteringSystemAtOmegaK:
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'''
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'''
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Wrapper over the C qpms_scatsys_at_omega_k_t structure
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Wrapper over the C qpms_scatsys_at_omega_k_t structure
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This represents an infinite periodic system with a given (fixed) frequency and Bloch vector.
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'''
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'''
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cdef qpms_scatsys_at_omega_k_t sswk
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cdef qpms_scatsys_at_omega_k_t sswk
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cdef _ScatteringSystemAtOmega ssw_pyref
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cdef _ScatteringSystemAtOmega ssw_pyref
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@ -1018,7 +1023,22 @@ cdef class _ScatteringSystemAtOmegaK:
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self.sswk.eta = eta
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self.sswk.eta = eta
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@boundscheck(False)
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@boundscheck(False)
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def scattered_E(self, scatcoeffvector_full, evalpos, btyp=QPMS_HANKEL_PLUS): # TODO DOC!!!
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def scattered_E(self, scatcoeffvector_full, evalpos, btyp=QPMS_HANKEL_PLUS):
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"""Evaluate electric field for a given excitation coefficient vector (periodic system)
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Parameters
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----------
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scatcoeffvector_full: array_like of shape (self.fecv_size,)
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Onedimensional excitation coefficient vector, describing SVWFs leaving
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the scatterers inside the representative unit cell.
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evalpos: array_like of floats and shape (..., 3)
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Evaluation points in cartesian coordinates.
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Returns
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-------
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array_like of complex, with the same shape as `evalpos`
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Electric field at the positions given in `evalpos`.
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"""
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if(btyp != QPMS_HANKEL_PLUS):
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if(btyp != QPMS_HANKEL_PLUS):
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raise NotImplementedError("Only first kind Bessel function-based fields are supported")
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raise NotImplementedError("Only first kind Bessel function-based fields are supported")
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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@ -1026,7 +1046,7 @@ cdef class _ScatteringSystemAtOmegaK:
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if evalpos.shape[-1] != 3:
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if evalpos.shape[-1] != 3:
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raise ValueError("Last dimension of evalpos has to be 3")
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raise ValueError("Last dimension of evalpos has to be 3")
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, copy=False)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, dtype=complex, copy=False)
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cdef cdouble[::1] scv_view = scv
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cdef cdouble[::1] scv_view = scv
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef ccart3_t res
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cdef ccart3_t res
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@ -1043,6 +1063,9 @@ cdef class _ScatteringSystemAtOmegaK:
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results[i,2] = res.z
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results[i,2] = res.z
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return results.reshape(evalpos.shape)
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return results.reshape(evalpos.shape)
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property fecv_size:
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def __get__(self): return self.ssw_pyref.ss_pyref.fecv_size
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cdef class _ScatteringSystemAtOmega:
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cdef class _ScatteringSystemAtOmega:
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'''
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'''
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Wrapper over the C qpms_scatsys_at_omega_t structure
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Wrapper over the C qpms_scatsys_at_omega_t structure
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@ -1097,6 +1120,7 @@ cdef class _ScatteringSystemAtOmega:
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def _sswk(self, k):
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def _sswk(self, k):
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cdef _ScatteringSystemAtOmegaK sswk = _ScatteringSystemAtOmegaK()
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cdef _ScatteringSystemAtOmegaK sswk = _ScatteringSystemAtOmegaK()
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sswk.sswk.ssw = self.ssw
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sswk.sswk.ssw = self.ssw
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sswk.ssw_pyref=self
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sswk.sswk.k[0] = k[0]
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sswk.sswk.k[0] = k[0]
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sswk.sswk.k[1] = k[1]
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sswk.sswk.k[1] = k[1]
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sswk.sswk.k[2] = k[2]
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sswk.sswk.k[2] = k[2]
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@ -1164,13 +1188,39 @@ cdef class _ScatteringSystemAtOmega:
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return self.ss_pyref.translation_matrix_packed(wavenumber=self.wavenumber, iri=iri, J=J)
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return self.ss_pyref.translation_matrix_packed(wavenumber=self.wavenumber, iri=iri, J=J)
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@boundscheck(False)
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@boundscheck(False)
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def scattered_E(self, scatcoeffvector_full, evalpos, bint alt=False, btyp=QPMS_HANKEL_PLUS):
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def scattered_E(self, scatcoeffvector_full, evalpos, blochvector=None, btyp=QPMS_HANKEL_PLUS, bint alt=False):
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# FIXME TODO this obviously does not work for periodic systems
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"""Evaluate electric field for a given excitation coefficient vector
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Parameters
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----------
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scatcoeffvector_full: array_like of shape (self.fecv_size,)
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Onedimensional excitation coefficient vector, describing SVWFs leaving
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the scatterers.
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evalpos: array_like of floats and shape (..., 3)
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Evaluation points in cartesian coordinates.
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blochvector: array_like or None
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Bloch vector, must be supplied (non-None) for periodic systems, else None.
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Returns
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-------
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array_like of complex, with the same shape as `evalpos`
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Electric field at the positions given in `evalpos`.
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See Also
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--------
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_ScatteringSystemAtOmegaK.scattered_E: Evaluate scattered field in an infinite periodic system.
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"""
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if(self.ssw[0].ss[0].lattice_dimension != 0):
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if blochvector is None:
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raise ValueError("For a periodic system, blochvector must be specified.")
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return self._sswk(blochvector).scattered_E(scatcoeffvector_full, evalpos=evalpos, btyp=btyp)
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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cdef qpms_bessel_t btyp_c = BesselType(btyp)
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evalpos = np.array(evalpos, dtype=float, copy=False)
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evalpos = np.array(evalpos, dtype=float, copy=False)
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if evalpos.shape[-1] != 3:
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if evalpos.shape[-1] != 3:
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raise ValueError("Last dimension of evalpos has to be 3")
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raise ValueError("Last dimension of evalpos has to be 3")
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[double,ndim=2] evalpos_a = evalpos.reshape(-1,3)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, copy=False)
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cdef np.ndarray[dtype=complex, ndim=1] scv = np.array(scatcoeffvector_full, dtype=complex, copy=False)
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cdef cdouble[::1] scv_view = scv
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cdef cdouble[::1] scv_view = scv
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef np.ndarray[complex, ndim=2] results = np.empty((evalpos_a.shape[0],3), dtype=complex)
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cdef ccart3_t res
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cdef ccart3_t res
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