2 Common snippets for argument processing in command line scripts; legacy scripts use scripts_common.py instead.
12 if isinstance(S
[0], list):
13 return flatten(S
[0]) + flatten(S
[1:])
14 return S
[:1] + flatten(S
[1:])
16 def make_action_sharedlist(opname
, listname
):
17 class opAction(argparse
.Action
):
18 def __call__(self
, parser
, args
, values
, option_string
=None):
19 if (not hasattr(args
, listname
)) or getattr(args
, listname
) is None:
20 setattr(args
, listname
, list())
21 getattr(args
, listname
).append((opname
, values
))
24 def make_dict_action(argtype
=None, postaction
='store', first_is_key
=True):
25 class DictAction(argparse
.Action
):
26 #def __init__(self, option_strings, dest, nargs=None, **kwargs):
27 # if nargs is not None:
28 # raise ValueError("nargs not allowed")
29 # super(DictAction, self).__init__(option_strings, dest, **kwargs)
30 def __call__(self
, parser
, namespace
, values
, option_string
=None):
31 if first_is_key
: # For the labeled versions
34 else: # For the default values
37 if argtype
is not None:
38 if (first_is_key
and self
.nargs
== 2) or (not first_is_key
and self
.nargs
== 1):
39 vals
= argtype(vals
[0]) # avoid having lists in this case
41 vals
= [argtype(val
) for val
in vals
]
42 ledict
= getattr(namespace
, self
.dest
, {})
45 if postaction
=='store':
47 elif postaction
=='append':
48 lelist
= ledict
.get(key
, [])
51 setattr(namespace
, self
.dest
, ledict
)
55 class ArgumentProcessingError(Exception):
58 class AppendTupleAction(argparse
.Action
):
59 ''' A variation on the 'append' builtin action from argparse, but uses tuples for the internal groupings instead of lists '''
60 def __call__(self
, parser
, args
, values
, option_string
=None):
61 if (not hasattr(args
, self
.dest
)) or getattr(args
, self
.dest
) is None:
62 setattr(args
, self
.dest
, list())
63 getattr(args
, self
.dest
).append(tuple(values
))
65 def float_range(string
):
66 """Tries to parse a string either as one individual float value
67 or one of the following patterns:
73 (The last one is equivalent to first:last|50.)
74 Returns either float or numpy array.
82 match
= re
.match(r
's?([^:]+):([^|]+)\|(.+)', string
)
84 steps
= int(match
.group(3))
86 match
= re
.match(r
's?([^:]+):([^:]+):(.+)', string
)
88 increment
= float(match
.group(3))
90 match
= re
.match(r
's?([^:]+):(.+)', string
)
94 argparse
.ArgumentTypeError('Invalid float/sequence format: "%s"' % string
)
95 first
= float(match
.group(1))
96 last
= float(match
.group(2))
99 return np
.linspace(first
, last
, num
=steps
)
101 return np
.arange(first
, last
, increment
)
103 def int_or_None(string
):
104 """Tries to parse a string either as an int or None (if it contains only whitespaces)"""
107 except ValueError as ve
:
108 if string
.strip() == '':
114 """Tries to parse a string either as one individual int value
115 or one of the following patterns:
120 first, last and increment must be parseable as ints
123 In each case, 's' letter can be prepended to the whole string to avoid
124 argparse interpreting this as a new option (if the argument contains
127 Returns either int or slice containing ints or Nones.
136 match
= re
.match(r
'([^:]*):([^:]*):(.*)', string
)
138 step
= int_or_None(match
.group(3))
140 match
= re
.match(r
'([^:]*):(.*)', string
)
144 argparse
.ArgumentTypeError('Invalid int/slice format: "%s"' % string
)
145 start
= int_or_None(match
.group(1))
146 stop
= int_or_None(match
.group(2))
147 return slice(start
, stop
, step
)
150 '''Tries to match a float, or a float with prepended 's'
152 Used as a workaraound for argparse's negative number matcher, which does not recognize
157 except ValueError as exc
:
159 res
= float(string
[1:])
164 '''Tries to match an int, or an int with prepended 's'
166 Used as a workaraound for argparse's negative number matcher if '+' is used as a
171 except ValueError as exc
:
173 res
= int(string
[1:])
177 def material_spec(string
):
178 """Tries to parse a string as a material specification, i.e. a
179 real or complex number or one of the string in built-in Lorentz-Drude models.
181 Tries to interpret the string as 1) float, 2) complex, 3) Lorentz-Drude key.
182 Raises argparse.ArgumentTypeError on failure.
184 from .cymaterials
import lorentz_drude
185 if string
in lorentz_drude
.keys():
188 try: lemat
= float(string
)
190 try: lemat
= complex(string
)
191 except ValueError as ve
:
192 raise argpares
.ArgumentTypeError("Material specification must be a supported material name %s, or a number" % (str(lorentz_drude
.keys()),)) from ve
196 ''' Common argument parsing engine for QPMS python CLI scripts. '''
198 def __add_planewave_argparse_group(ap
):
199 pwgrp
= ap
.add_argument_group('Incident wave specification', """
200 Incident wave direction is given in terms of ISO polar and azimuthal angles θ, φ,
201 which translate into cartesian coordinates as r̂ = (x, y, z) = (sin(θ) cos(φ), sin(θ) sin(φ), cos(θ)).
203 Wave polarisation is given in terms of parameters ψ, χ, where ψ is the angle between a polarisation
204 ellipse axis and meridian tangent θ̂, and tg χ determines axes ratio;
205 the electric field in the origin is then
207 E⃗ = cos(χ) (cos(ψ) θ̂ + sin(ψ) φ̂) + i sin(χ) (sin(ψ) θ̂ + cos(ψ) φ̂).
209 All the angles are given as multiples of π/2.
212 pwgrp
.add_argument("-φ", "--phi", type=float, default
=0,
213 help='Incident wave asimuth in multiples of π/2.')
214 pwgrp
.add_argument("-θ", "--theta", type=float_range
, default
=0,
215 help='Incident wave polar angle in multiples of π/2. This might be a sequence in format FIRST:LAST:INCREMENT.')
216 pwgrp
.add_argument("-ψ", "--psi", type=float, default
=0,
217 help='Angle between polarisation ellipse axis and meridian tangent θ̂ in multiples of π/2.')
218 pwgrp
.add_argument("-χ", "--chi", type=float, default
=0,
219 help='Polarisation parameter χ in multiples of π/2. 0 for linear, 0.5 for circular pol.')
221 def __add_manyparticle_argparse_group(ap
):
222 mpgrp
= ap
.add_argument_group('Many particle specification', "TODO DOC")
223 mpgrp
.add_argument("-p", "--position", nargs
='+', action
=make_dict_action(argtype
=sfloat
, postaction
='append',
224 first_is_key
=False), help="Particle positions, cartesion coordinates (default particle properties)")
225 mpgrp
.add_argument("+p", "++position", nargs
='+', action
=make_dict_action(argtype
=sfloat
, postaction
='append',
226 first_is_key
=True), help="Particle positions, cartesian coordinates (labeled)")
227 mpgrp
.add_argument("-L", "--lMax", nargs
=1, default
={},
228 action
=make_dict_action(argtype
=int, postaction
='store', first_is_key
=False,),
229 help="Cutoff multipole degree (default)")
230 mpgrp
.add_argument("+L", "++lMax", nargs
=2,
231 action
=make_dict_action(argtype
=int, postaction
='store', first_is_key
=True,),
232 help="Cutoff multipole degree (labeled)")
233 mpgrp
.add_argument("-m", "--material", nargs
=1, default
={},
234 action
=make_dict_action(argtype
=material_spec
, postaction
='store', first_is_key
=False,),
235 help='particle material (Au, Ag, ... for Lorentz-Drude or number for constant refractive index) (default)')
236 mpgrp
.add_argument("+m", "++material", nargs
=2,
237 action
=make_dict_action(argtype
=material_spec
, postaction
='store', first_is_key
=True,),
238 help='particle material (Au, Ag, ... for Lorentz-Drude or number for constant refractive index) (labeled)')
239 mpgrp
.add_argument("-r", "--radius", nargs
=1, default
={},
240 action
=make_dict_action(argtype
=float, postaction
='store', first_is_key
=False,),
241 help='particle radius (sphere or cylinder; default)')
242 mpgrp
.add_argument("+r", "++radius", nargs
=2,
243 action
=make_dict_action(argtype
=float, postaction
='store', first_is_key
=True,),
244 help='particle radius (sphere or cylinder; labeled)')
245 mpgrp
.add_argument("-H", "--height", nargs
=1, default
={},
246 action
=make_dict_action(argtype
=float, postaction
='store', first_is_key
=False,),
247 help='particle radius (cylinder; default)')
248 mpgrp
.add_argument("+H", "++height", nargs
=2,
249 action
=make_dict_action(argtype
=float, postaction
='store', first_is_key
=True,),
250 help='particle radius (cylinder; labeled)')
253 'rectlattice2d_periods': lambda ap
: ap
.add_argument("-p", "--period", type=float, nargs
='+', required
=True, help='square/rectangular lattice periods', metavar
=('px','[py]')),
254 'rectlattice2d_counts': lambda ap
: ap
.add_argument("--size", type=int, nargs
=2, required
=True, help='rectangular array size (particle column, row count)', metavar
=('NCOLS', 'NROWS')),
255 'single_frequency_eV': lambda ap
: ap
.add_argument("-f", "--eV", type=float, required
=True, help='radiation angular frequency in eV'),
256 'multiple_frequency_eV_optional': lambda ap
: ap
.add_argument("-f", "--eV", type=float, nargs
='*', help='radiation angular frequency in eV (additional)'),
257 'seq_frequency_eV': lambda ap
: ap
.add_argument("-F", "--eV-seq", type=float, nargs
=3, required
=True, help='uniform radiation angular frequency sequence in eV', metavar
=('FIRST', 'INCREMENT', 'LAST')),
258 'real_frequencies_eV_ng': lambda ap
: ap
.add_argument("-f", "--eV", type=float_range
, nargs
=1, action
='append', required
=True, help='Angular frequency (or angular frequency range) in eV'), # nargs='+', action='extend' would be better, but action='extend' requires python>=3.8
259 'single_material': lambda ap
: ap
.add_argument("-m", "--material", help='particle material (Au, Ag, ... for Lorentz-Drude or number for constant refractive index)', type=material_spec
, required
=True),
260 'single_radius': lambda ap
: ap
.add_argument("-r", "--radius", type=float, required
=True, help='particle radius (sphere or cylinder)'),
261 'single_height': lambda ap
: ap
.add_argument("-H", "--height", type=float, help='cylindrical particle height; if not provided, particle is assumed to be spherical'),
262 'single_kvec2': lambda ap
: ap
.add_argument("-k", '--kx-lim', nargs
=2, type=sfloat
, required
=True, help='k vector', metavar
=('KX_MIN', 'KX_MAX')),
263 'kpi': lambda ap
: ap
.add_argument("--kpi", action
='store_true', help="Indicates that the k vector is given in natural units instead of SI, i.e. the arguments given by -k shall be automatically multiplied by pi / period (given by -p argument)"),
264 'bg_real_refractive_index': lambda ap
: ap
.add_argument("-n", "--refractive-index", type=float, default
=1., help='background medium strictly real refractive index'),
265 'bg_analytical': lambda ap
: ap
.add_argument("-B", "--background", type=material_spec
, default
=1., help="Background medium specification (constant real or complex refractive index, or supported material label)"),
266 'single_lMax': lambda ap
: ap
.add_argument("-L", "--lMax", type=int, required
=True, default
=3, help='multipole degree cutoff'),
267 'single_lMax_extend': lambda ap
: ap
.add_argument("--lMax-extend", type=int, required
=False, default
=6, help='multipole degree cutoff for T-matrix calculation (cylindrical particles only'),
268 'outfile': lambda ap
: ap
.add_argument("-o", "--output", type=str, required
=False, help='output path (if not provided, will be generated automatically)'), # TODO consider type=argparse.FileType('w')
269 'plot_out': lambda ap
: ap
.add_argument("-O", "--plot-out", type=str, required
=False, help="path to plot output (optional)"),
270 'plot_do': lambda ap
: ap
.add_argument("-P", "--plot", action
='store_true', help="if -p not given, plot to a default path"),
271 'lattice2d_basis': lambda ap
: ap
.add_argument("-b", "--basis-vector", nargs
='+', action
=AppendTupleAction
, help="basis vector in xy-cartesian coordinates (two required)", required
=True, type=sfloat
, dest
='basis_vectors', metavar
=('X', 'Y')),
272 'planewave_pol_angles': __add_planewave_argparse_group
,
273 'multi_particle': __add_manyparticle_argparse_group
,
276 feature_sets_available
= { # name : (description, dependencies, atoms not in other dependencies, methods called after parsing, "virtual" features provided)
277 'const_real_background': ("Background medium with constant real refractive index", (), ('bg_real_refractive_index',), ('_eval_const_background_epsmu',), ('background', 'background_analytical')),
278 'background' : ("Most general background medium specification currently supported", ('background_analytical',), (), (), ()),
279 'background_analytical' : ("Background medium model holomorphic for 'reasonably large' complex frequency areas", (), ('bg_analytical',), ('_eval_analytical_background_epsmugen',), ('background',)),
280 'single_particle': ("Single particle definition (shape [currently spherical or cylindrical]) and materials, incl. background)", ('background',), ('single_material', 'single_radius', 'single_height', 'single_lMax_extend'), ('_eval_single_tmgen',), ()),
281 'multi_particle': ("One or more particle definition (shape [curently spherical or cylindrical]), materials, and positions)", ('background',), ('multi_particle',), ('_process_multi_particle',), ()),
282 'single_lMax': ("Single particle lMax definition", (), ('single_lMax',), (), ()),
283 'single_omega': ("Single angular frequency", (), ('single_frequency_eV',), ('_eval_single_omega',), ()),
284 'omega_seq': ("Equidistant real frequency range with possibility of adding individual frequencies", (), ('seq_frequency_eV', 'multiple_frequency_eV_optional',), ('_eval_omega_seq',), ()),
285 'omega_seq_real_ng': ("Equidistant real frequency ranges or individual frequencies (new syntax)", (), ('real_frequencies_eV_ng',), ('_eval_omega_seq_real_ng',), ()),
286 'lattice2d': ("Specification of a generic 2d lattice (spanned by the x,y axes)", (), ('lattice2d_basis',), ('_eval_lattice2d',), ()),
287 'rectlattice2d': ("Specification of a rectangular 2d lattice; conflicts with lattice2d", (), ('rectlattice2d_periods',), ('_eval_rectlattice2d',), ()),
288 'rectlattice2d_finite': ("Specification of a rectangular 2d lattice; conflicts with lattice2d", ('rectlattice2d',), ('rectlattice2d_counts',), (), ()),
289 'planewave': ("Specification of a normalised plane wave (typically used for scattering) with a full polarisation state", (), ('planewave_pol_angles',), ("_process_planewave_angles",), ()),
293 def __init__(self
, features
=[]):
294 prefix_chars
= '+-' if 'multi_particle' in features
else '-'
295 self
.ap
= argparse
.ArgumentParser(prefix_chars
=prefix_chars
)
296 self
.features_enabled
= set()
297 self
.call_at_parse_list
= []
299 for feat
in features
:
300 self
.add_feature(feat
)
301 self
._emg
_register
= {} # EpsMuGenerator dictionary to avoid recreating equivalent instances; filled by _add_emg()
302 self
._tmg
_register
= {} # TMatrixGenerator dictionary to avoid recreating equivalent instances; filled by _add_tmg()
303 self
._bspec
_register
= {} # Dictionary of used BaseSpecs to keep the equivalent instances unique; filled by _add_bspec()
305 def _add_emg(self
, emgspec
):
306 """Looks up whether if an EpsMuGenerator from given material_spec has been already registered, and if not, creates a new one"""
307 from .cymaterials
import EpsMu
, EpsMuGenerator
, lorentz_drude
308 if emgspec
in self
._emg
_register
.keys():
309 return self
._emg
_register
[emgspec
]
311 if isinstance(emgspec
, (float, complex)):
312 emg
= EpsMuGenerator(EpsMu(emgspec
**2))
314 emg
= EpsMuGenerator(lorentz_drude
[emgspec
])
315 self
._emg
_register
[emgspec
] = emg
318 def _add_tmg(self
, tmgspec
):
319 """Looks up whether if a T-matrix from given T-matrix specification tuple has been already registered, and if not, creates a new one
321 T-matrix specification shall be of the form
322 (bg_material_spec, fg_material_spec, shape_spec) where shape_spec is
323 (radius, height, lMax_extend)
325 if tmgspec
in self
._tmg
_register
.keys():
326 return self
._tmg
_register
[tmgspec
]
328 from .cytmatrices
import TMatrixGenerator
329 bgspec
, fgspec
, (radius
, height
, lMax_extend
) = tmgspec
330 bg
= self
._add
_emg
(bgspec
)
331 fg
= self
._add
_emg
(fgspec
)
333 tmgen
= TMatrixGenerator
.sphere(bg
, fg
, radius
)
335 tmgen
= TMatrixGenerator
.cylinder(bg
, fg
, radius
, height
, lMax_extend
=lMax_extend
)
336 self
._tmg
_register
[tmgspec
] = tmgen
339 def _add_bspec(self
, key
):
340 if key
in self
._bspec
_register
.keys():
341 return self
._bspec
_register
[key
]
343 from .cybspec
import BaseSpec
344 if isinstance(key
, BaseSpec
):
346 elif isinstance(key
, int):
347 bspec
= self
._add
_bspec
(BaseSpec(lMax
=key
))
348 else: raise TypeError("Can't register this as a BaseSpec")
349 self
._bspec
_register
[key
] = bspec
352 def add_feature(self
, feat
):
353 if feat
not in self
.features_enabled
:
354 if feat
not in ArgParser
.feature_sets_available
:
355 raise ValueError("Unknown ArgParser feature: %s" % feat
)
356 #resolve dependencies
357 _
, deps
, atoms
, atparse
, provides_virtual
= ArgParser
.feature_sets_available
[feat
]
359 self
.add_feature(dep
)
360 for atom
in atoms
: # maybe check whether that atom has already been added sometimes in the future?
361 ArgParser
.atomic_arguments
[atom
](self
.ap
)
362 for methodname
in atparse
:
363 self
.call_at_parse_list
.append(methodname
)
364 self
.features_enabled
.add(feat
)
365 for feat_virt
in provides_virtual
:
366 self
.features_enabled
.add(feat_virt
)
368 def add_argument(self
, *args
, **kwargs
):
369 '''Add a custom argument directly to the standard library ArgParser object'''
370 return self
.ap
.add_argument(*args
, **kwargs
)
372 def add_argument_group(self
, *args
, **kwargs
):
373 '''Add a custom argument group directly to the standard library ArgParser object'''
374 return self
.ap
.add_argument_group(*args
, **kwargs
)
376 def parse_args(self
, process_data
= True, *args
, **kwargs
):
377 self
.args
= self
.ap
.parse_args(*args
, **kwargs
)
379 for method
in self
.call_at_parse_list
:
381 getattr(self
, method
)()
382 except ArgumentProcessingError
:
383 err
= sys
.exc_info()[1]
384 self
.ap
.error(str(err
))
387 def __getattr__(self
, name
):
388 return getattr(self
.args
, name
)
391 # Methods to initialise the related data structures:
393 def _eval_const_background_epsmu(self
): # feature: const_real_background
394 self
.args
.background
= self
.args
.refractive_index
395 self
._eval
_analytical
_background
_epsmugen
()
397 def _eval_analytical_background_epsmugen(self
): # feature: background_analytical
399 from .cymaterials
import EpsMu
400 if isinstance(a
.background
, (float, complex)):
401 self
.background_epsmu
= EpsMu(a
.background
**2)
402 self
.background_emg
= self
._add
_emg
(a
.background
)
404 def _eval_single_tmgen(self
): # feature: single_particle
406 from .cymaterials
import EpsMuGenerator
, lorentz_drude
407 from .cytmatrices
import TMatrixGenerator
408 self
.foreground_emg
= self
._add
_emg
(a
.material
)
409 self
.tmgen
= self
._add
_tmg
((a
.background
, a
.material
, (a
.radius
, a
.height
, a
.lMax_extend
)))
410 self
.bspec
= self
._add
_bspec
(a
.lMax
)
412 def _eval_single_omega(self
): # feature: single_omega
413 from .constants
import eV
, hbar
414 self
.omega
= self
.args
.eV
* eV
/ hbar
416 def _eval_omega_seq(self
): # feature: omega_seq
418 from .constants
import eV
, hbar
419 start
, step
, stop
= self
.args
.eV_seq
420 self
.omegas
= np
.arange(start
, stop
, step
)
422 self
.omegas
= np
.concatenate((self
.omegas
, np
.array(self
.args
.eV
)))
424 self
.omegas
*= eV
/hbar
426 def _eval_omega_seq_real_ng(self
): # feature: omega_seq_real_ng
428 from .constants
import eV
, hbar
430 self
.omegas
= [omega_eV
* eh
for omega_eV
in flatten(self
.args
.eV
)]
431 self
.omega_max
= max(om
if isinstance(om
, float) else max(om
) for om
in self
.omegas
)
432 self
.omega_min
= min(om
if isinstance(om
, float) else min(om
) for om
in self
.omegas
)
433 self
.omega_singles
= [om
for om
in self
.omegas
if isinstance(om
, float)]
434 self
.omega_ranges
= [om
for om
in self
.omegas
if not isinstance(om
, float)]
435 self
.omega_descr
= ("%geV" % (self
.omega_max
/ eh
)) if (self
.omega_max
== self
.omega_min
) else (
436 "%g–%geV" % (self
.omega_min
/ eh
, self
.omega_max
/ eh
))
438 for om
in self
.omegas
:
439 if isinstance(om
, float):
440 self
.allomegas
.append(om
)
442 self
.allomegas
.extend(om
)
443 self
.allomegas
= np
.unique(self
.allomegas
)
446 def _eval_lattice2d(self
): # feature: lattice2d
447 l
= len(self
.args
.basis_vectors
)
448 if l
!= 2: raise ValueError('Two basis vectors must be specified (have %d)' % l
)
449 from .qpms_c
import lll_reduce
450 self
.direct_basis
= lll_reduce(self
.args
.basis_vectors
, delta
=1.)
452 self
.reciprocal_basis1
= np
.linalg
.inv(self
.direct_basis
.T
)
453 self
.reciprocal_basis2pi
= 2 * np
.pi
* self
.reciprocal_basis1
455 def _eval_rectlattice2d(self
): # feature: rectlattice2d
458 if (l
== 1): # square lattice
459 a
.period
= (a
.period
[0], a
.period
[0])
461 a
.period
= (a
.period
[0], a
.period
[1])
463 raise ValueError("At most two lattice periods allowed for a rectangular lattice (got %d)" % l
)
466 a
.basis_vectors
= [(a
.period
[0], 0.), (0., a
.period
[1])]
467 self
.direct_basis
= np
.array(a
.basis_vectors
)
468 self
.reciprocal_basis1
= np
.linalg
.inv(self
.direct_basis
.T
)
469 self
.reciprocal_basis2pi
= 2 * np
.pi
* self
.reciprocal_basis1
471 def _process_planewave_angles(self
): #feature: planewave
477 a
.theta
= a
.theta
* pi2
480 def _process_multi_particle(self
): # feature: multi_particle
486 pos13
, pos23
, pos33
= False, False, False # used to
487 if len(a
.position
.keys()) == 0:
488 warnings
.warn("No particle position (-p or +p) specified, assuming single particle in the origin / single particle per unit cell!")
489 a
.position
[None] = [(0.,0.,0.)]
490 for poslabel
in a
.position
.keys():
492 lMax
= a
.lMax
.get(poslabel
, False) or a
.lMax
[None]
493 radius
= a
.radius
.get(poslabel
, False) or a
.radius
[None]
494 # Height is "inherited" only together with radius
495 height
= a
.height
.get(poslabel
, None) if poslabel
in a
.radius
.keys() else a
.height
.get(None, None)
496 if hasattr(a
, 'lMax_extend'):
497 lMax_extend
= a
.lMax_extend
.get(poslabel
, False) or a
.lMax_extend
.get(None, False) or None
500 material
= a
.material
.get(poslabel
, False) or a
.material
[None]
501 except (TypeError, KeyError) as exc
:
503 raise ArgumentProcessingError("Unlabeled particles' positions (-p) specified, but some default particle properties are missing (--lMax, --radius, and --material have to be specified)") from exc
505 raise ArgumentProcessingError(("Incomplete specification of '%s'-labeled particles: you must"
506 "provide at least ++lMax, ++radius, ++material arguments with the label, or the fallback arguments"
507 "--lMax, --radius, --material.")%(str(poslabel
),)) from exc
508 tmspec
= (a
.background
, material
, (radius
, height
, lMax_extend
))
509 self
.tmspecs
[poslabel
] = tmspec
510 self
.tmgens
[poslabel
] = self
._add
_tmg
(tmspec
)
511 self
.bspecs
[poslabel
] = self
._add
_bspec
(lMax
)
513 for pos
in a
.position
[poslabel
]:
515 pos_cured
= (0., 0., pos
[0])
518 pos_cured
= (pos
[0], pos
[1], 0.)
524 raise argparse
.ArgumentTypeError("Each -p / +p argument requires 1 to 3 cartesian coordinates")
525 poslist_cured
.append(pos_cured
)
526 self
.positions
[poslabel
] = poslist_cured
528 warnings
.warn("Both 1D and 2D position specifications used. The former are interpreted as z coordinates while the latter as x, y coordinates")
530 def get_particles(self
):
531 """Creates a list of Particle instances that can be directly used in ScatteringSystem.create().
533 Assumes that self._process_multi_particle() has been already called.
535 from .qpms_c
import Particle
537 for poslabel
, poss
in self
.positions
.items():
538 t
= self
.tmgens
[poslabel
]
539 bspec
= self
.bspecs
[poslabel
]
540 plist
.extend([Particle(pos
, t
, bspec
=bspec
) for pos
in poss
])