invertor.py @ 3641881

ESS_GUIESS_GUI_DocsESS_GUI_batch_fittingESS_GUI_bumps_abstractionESS_GUI_iss1116ESS_GUI_iss879ESS_GUI_iss959ESS_GUI_openclESS_GUI_orderingESS_GUI_sync_sascalccostrafo411magnetic_scattrelease-4.1.1release-4.1.2release-4.2.2release_4.0.1ticket-1009ticket-1094-headlessticket-1242-2d-resolutionticket-1243ticket-1249ticket885unittest-saveload

Last change on this file since 3641881 was d84a90c, checked in by Gervaise Alina <gervyh@…>, 14 years ago
working on documentation
Property mode set to `100644`
File size: 25.2 KB

Line
1	"""
2	Module to perform P(r) inversion.
3	The module contains the Invertor class.
4	"""
5	from sans.pr.core.pr_inversion import Cinvertor
6	import numpy
7	import sys
8	import math, time
9	from numpy.linalg import lstsq
10
11	def help():
12	"""
13	Provide general online help text
14	Future work: extend this function to allow topic selection
15	"""
16	info_txt = "The inversion approach is based on Moore, J. Appl. Cryst. (1980) 13, 168-175.\n\n"
17	info_txt += "P(r) is set to be equal to an expansion of base functions of the type "
18	info_txt += "phi_n(r) = 2rsin(pinr/D_max). The coefficient of each base functions "
19	info_txt += "in the expansion is found by performing a least square fit with the "
20	info_txt += "following fit function:\n\n"
21	info_txt += "chi2 = sum_i[ I_meas(q_i) - I_th(q_i) ]2/error**2 + Reg_term\n\n"
22	info_txt += "where I_meas(q) is the measured scattering intensity and I_th(q) is "
23	info_txt += "the prediction from the Fourier transform of the P(r) expansion. "
24	info_txt += "The Reg_term term is a regularization term set to the second derivative "
25	info_txt += "d2P(r)/dr2 integrated over r. It is used to produce a smooth P(r) output.\n\n"
26	info_txt += "The following are user inputs:\n\n"
27	info_txt += " - Number of terms: the number of base functions in the P(r) expansion.\n\n"
28	info_txt += " - Regularization constant: a multiplicative constant to set the size of "
29	info_txt += "the regularization term.\n\n"
30	info_txt += " - Maximum distance: the maximum distance between any two points in the system.\n"
31
32	return info_txt
33
34
35	class Invertor(Cinvertor):
36	"""
37	Invertor class to perform P(r) inversion
38
39	The problem is solved by posing the problem as Ax = b,
40	where x is the set of coefficients we are looking for.
41
42	Npts is the number of points.
43
44	In the following i refers to the ith base function coefficient.
45	The matrix has its entries j in its first Npts rows set to
46	A[j][i] = (Fourier transformed base function for point j)
47
48	We them choose a number of r-points, n_r, to evaluate the second
49	derivative of P(r) at. This is used as our regularization term.
50	For a vector r of length n_r, the following n_r rows are set to
51	A[j+Npts][i] = (2nd derivative of P(r), d2(P(r))/d(r)2, evaluated at r[j])
52
53	The vector b has its first Npts entries set to
54	b[j] = (I(q) observed for point j)
55
56	The following n_r entries are set to zero.
57
58	The result is found by using scipy.linalg.basic.lstsq to invert
59	the matrix and find the coefficients x.
60
61	Methods inherited from Cinvertor:
62	- get_peaks(pars): returns the number of P(r) peaks
63	- oscillations(pars): returns the oscillation parameters for the output P(r)
64	- get_positive(pars): returns the fraction of P(r) that is above zero
65	- get_pos_err(pars): returns the fraction of P(r) that is 1-sigma above zero
66	"""
67	## Chisqr of the last computation
68	chi2 = 0
69	## Time elapsed for last computation
70	elapsed = 0
71	## Alpha to get the reg term the same size as the signal
72	suggested_alpha = 0
73	## Last number of base functions used
74	nfunc = 10
75	## Last output values
76	out = None
77	## Last errors on output values
78	cov = None
79	## Background value
80	background = 0
81	## Information dictionary for application use
82	info = {}
83
84
85	def __init__(self):
86	Cinvertor.__init__(self)
87
88	def __setattr__(self, name, value):
89	"""
90	Set the value of an attribute.
91	Access the parent class methods for
92	x, y, err, d_max, q_min, q_max and alpha
93	"""
94	if name=='x':
95	if 0.0 in value:
96	raise ValueError, "Invertor: one of your q-values is zero. Delete that entry before proceeding"
97	return self.set_x(value)
98	elif name=='y':
99	return self.set_y(value)
100	elif name=='err':
101	value2 = abs(value)
102	return self.set_err(value2)
103	elif name=='d_max':
104	return self.set_dmax(value)
105	elif name=='q_min':
106	if value==None:
107	return self.set_qmin(-1.0)
108	return self.set_qmin(value)
109	elif name=='q_max':
110	if value==None:
111	return self.set_qmax(-1.0)
112	return self.set_qmax(value)
113	elif name=='alpha':
114	return self.set_alpha(value)
115	elif name=='slit_height':
116	return self.set_slit_height(value)
117	elif name=='slit_width':
118	return self.set_slit_width(value)
119	elif name=='has_bck':
120	if value==True:
121	return self.set_has_bck(1)
122	elif value==False:
123	return self.set_has_bck(0)
124	else:
125	raise ValueError, "Invertor: has_bck can only be True or False"
126
127	return Cinvertor.__setattr__(self, name, value)
128
129	def __getattr__(self, name):
130	"""
131	Return the value of an attribute
132	"""
133	import numpy
134	if name=='x':
135	out = numpy.ones(self.get_nx())
136	self.get_x(out)
137	return out
138	elif name=='y':
139	out = numpy.ones(self.get_ny())
140	self.get_y(out)
141	return out
142	elif name=='err':
143	out = numpy.ones(self.get_nerr())
144	self.get_err(out)
145	return out
146	elif name=='d_max':
147	return self.get_dmax()
148	elif name=='q_min':
149	qmin = self.get_qmin()
150	if qmin<0:
151	return None
152	return qmin
153	elif name=='q_max':
154	qmax = self.get_qmax()
155	if qmax<0:
156	return None
157	return qmax
158	elif name=='alpha':
159	return self.get_alpha()
160	elif name=='slit_height':
161	return self.get_slit_height()
162	elif name=='slit_width':
163	return self.get_slit_width()
164	elif name=='has_bck':
165	value = self.get_has_bck()
166	if value==1:
167	return True
168	else:
169	return False
170	elif name in self.__dict__:
171	return self.__dict__[name]
172	return None
173
174	def clone(self):
175	"""
176	Return a clone of this instance
177	"""
178	import copy
179
180	invertor = Invertor()
181	invertor.chi2 = self.chi2
182	invertor.elapsed = self.elapsed
183	invertor.nfunc = self.nfunc
184	invertor.alpha = self.alpha
185	invertor.d_max = self.d_max
186	invertor.q_min = self.q_min
187	invertor.q_max = self.q_max
188
189	invertor.x = self.x
190	invertor.y = self.y
191	invertor.err = self.err
192	invertor.has_bck = self.has_bck
193	invertor.slit_height = self.slit_height
194	invertor.slit_width = self.slit_width
195
196	invertor.info = copy.deepcopy(self.info)
197
198	return invertor
199
200	def invert(self, nfunc=10, nr=20):
201	"""
202	Perform inversion to P(r)
203
204	The problem is solved by posing the problem as Ax = b,
205	where x is the set of coefficients we are looking for.
206
207	Npts is the number of points.
208
209	In the following i refers to the ith base function coefficient.
210	The matrix has its entries j in its first Npts rows set to
211	A[i][j] = (Fourier transformed base function for point j)
212
213	We them choose a number of r-points, n_r, to evaluate the second
214	derivative of P(r) at. This is used as our regularization term.
215	For a vector r of length n_r, the following n_r rows are set to
216	A[i+Npts][j] = (2nd derivative of P(r), d2(P(r))/d(r)2, evaluated at r[j])
217
218	The vector b has its first Npts entries set to
219	b[j] = (I(q) observed for point j)
220
221	The following n_r entries are set to zero.
222
223	The result is found by using scipy.linalg.basic.lstsq to invert
224	the matrix and find the coefficients x.
225
226	:param nfunc: number of base functions to use.
227	:param nr: number of r points to evaluate the 2nd derivative at for the reg. term.
228	:return: c_out, c_cov - the coefficients with covariance matrix
229
230	"""
231	# Reset the background value before proceeding
232	self.background = 0.0
233	return self.lstsq(nfunc, nr=nr)
234
235	def iq(self, out, q):
236	"""
237	Function to call to evaluate the scattering intensity
238
239	:param args: c-parameters, and q
240	:return: I(q)
241
242	"""
243	return Cinvertor.iq(self, out, q)+self.background
244
245	def invert_optimize(self, nfunc=10, nr=20):
246	"""
247	Slower version of the P(r) inversion that uses scipy.optimize.leastsq.
248
249	This probably produce more reliable results, but is much slower.
250	The minimization function is set to sum_i[ (I_obs(q_i) - I_theo(q_i))/err*2 ] + alpha reg_term,
251	where the reg_term is given by Svergun: it is the integral of the square of the first derivative
252	of P(r), d(P(r))/dr, integrated over the full range of r.
253
254	:param nfunc: number of base functions to use.
255	:param nr: number of r points to evaluate the 2nd derivative at for the reg. term.
256
257	:return: c_out, c_cov - the coefficients with covariance matrix
258
259	"""
260
261	from scipy import optimize
262	import time
263
264	self.nfunc = nfunc
265	# First, check that the current data is valid
266	if self.is_valid()<=0:
267	raise RuntimeError, "Invertor.invert: Data array are of different length"
268
269	p = numpy.ones(nfunc)
270	t_0 = time.time()
271	out, cov_x, info, mesg, success = optimize.leastsq(self.residuals, p, full_output=1, warning=True)
272
273	# Compute chi^2
274	res = self.residuals(out)
275	chisqr = 0
276	for i in range(len(res)):
277	chisqr += res[i]
278
279	self.chi2 = chisqr
280
281	# Store computation time
282	self.elapsed = time.time() - t_0
283
284	return out, cov_x
285
286	def pr_fit(self, nfunc=5):
287	"""
288	This is a direct fit to a given P(r). It assumes that the y data
289	is set to some P(r) distribution that we are trying to reproduce
290	with a set of base functions.
291
292	This method is provided as a test.
293	"""
294	from scipy import optimize
295
296	# First, check that the current data is valid
297	if self.is_valid()<=0:
298	raise RuntimeError, "Invertor.invert: Data arrays are of different length"
299
300	p = numpy.ones(nfunc)
301	t_0 = time.time()
302	out, cov_x, info, mesg, success = optimize.leastsq(self.pr_residuals, p, full_output=1, warning=True)
303
304	# Compute chi^2
305	res = self.pr_residuals(out)
306	chisqr = 0
307	for i in range(len(res)):
308	chisqr += res[i]
309
310	self.chisqr = chisqr
311
312	# Store computation time
313	self.elapsed = time.time() - t_0
314
315	return out, cov_x
316
317	def pr_err(self, c, c_cov, r):
318	"""
319	Returns the value of P(r) for a given r, and base function
320	coefficients, with error.
321
322	:param c: base function coefficients
323	:param c_cov: covariance matrice of the base function coefficients
324	:param r: r-value to evaluate P(r) at
325
326	:return: P(r)
327
328	"""
329	return self.get_pr_err(c, c_cov, r)
330
331	def _accept_q(self, q):
332	"""
333	Check q-value against user-defined range
334	"""
335	if not self.q_min==None and q<self.q_min:
336	return False
337	if not self.q_max==None and q>self.q_max:
338	return False
339	return True
340
341	def lstsq(self, nfunc=5, nr=20):
342	"""
343	The problem is solved by posing the problem as Ax = b,
344	where x is the set of coefficients we are looking for.
345
346	Npts is the number of points.
347
348	In the following i refers to the ith base function coefficient.
349	The matrix has its entries j in its first Npts rows set to
350	A[i][j] = (Fourier transformed base function for point j)
351
352	We them choose a number of r-points, n_r, to evaluate the second
353	derivative of P(r) at. This is used as our regularization term.
354	For a vector r of length n_r, the following n_r rows are set to
355	A[i+Npts][j] = (2nd derivative of P(r), d2(P(r))/d(r)2, evaluated at r[j])
356
357	The vector b has its first Npts entries set to
358	b[j] = (I(q) observed for point j)
359
360	The following n_r entries are set to zero.
361
362	The result is found by using scipy.linalg.basic.lstsq to invert
363	the matrix and find the coefficients x.
364
365	:param nfunc: number of base functions to use.
366	:param nr: number of r points to evaluate the 2nd derivative at for the reg. term.
367
368	If the result does not allow us to compute the covariance matrix,
369	a matrix filled with zeros will be returned.
370
371	"""
372	# Note: To make sure an array is contiguous:
373	# blah = numpy.ascontiguousarray(blah_original)
374	# ... before passing it to C
375
376	if self.is_valid()<0:
377	raise RuntimeError, "Invertor: invalid data; incompatible data lengths."
378
379	self.nfunc = nfunc
380	# a -- An M x N matrix.
381	# b -- An M x nrhs matrix or M vector.
382	npts = len(self.x)
383	nq = nr
384	sqrt_alpha = math.sqrt(math.fabs(self.alpha))
385	if sqrt_alpha<0.0:
386	nq = 0
387
388	# If we need to fit the background, add a term
389	if self.has_bck==True:
390	nfunc_0 = nfunc
391	nfunc += 1
392
393	a = numpy.zeros([npts+nq, nfunc])
394	b = numpy.zeros(npts+nq)
395	err = numpy.zeros([nfunc, nfunc])
396
397	# Construct the a matrix and b vector that represent the problem
398	t_0 = time.time()
399	self._get_matrix(nfunc, nq, a, b)
400
401	# Perform the inversion (least square fit)
402	c, chi2, rank, n = lstsq(a, b)
403	# Sanity check
404	try:
405	float(chi2)
406	except:
407	chi2 = -1.0
408	self.chi2 = chi2
409
410	inv_cov = numpy.zeros([nfunc,nfunc])
411	# Get the covariance matrix, defined as inv_cov = a_transposed * a
412	self._get_invcov_matrix(nfunc, nr, a, inv_cov)
413
414	# Compute the reg term size for the output
415	sum_sig, sum_reg = self._get_reg_size(nfunc, nr, a)
416
417	if math.fabs(self.alpha)>0:
418	new_alpha = sum_sig/(sum_reg/self.alpha)
419	else:
420	new_alpha = 0.0
421	self.suggested_alpha = new_alpha
422
423	try:
424	cov = numpy.linalg.pinv(inv_cov)
425	err = math.fabs(chi2/float(npts-nfunc)) * cov
426	except:
427	# We were not able to estimate the errors
428	# Return an empty error matrix
429	pass
430
431	# Keep a copy of the last output
432	if self.has_bck==False:
433	self.background = 0
434	self.out = c
435	self.cov = err
436	else:
437	self.background = c[0]
438
439	err_0 = numpy.zeros([nfunc, nfunc])
440	c_0 = numpy.zeros(nfunc)
441
442	for i in range(nfunc_0):
443	c_0[i] = c[i+1]
444	for j in range(nfunc_0):
445	err_0[i][j] = err[i+1][j+1]
446
447	self.out = c_0
448	self.cov = err_0
449
450	return self.out, self.cov
451
452	def estimate_numterms(self, isquit_func=None):
453	"""
454	Returns a reasonable guess for the
455	number of terms
456
457	:param isquit_func: reference to thread function to call to
458	check whether the computation needs to
459	be stopped.
460
461	:return: number of terms, alpha, message
462
463	"""
464	from num_term import Num_terms
465	estimator = Num_terms(self.clone())
466	try:
467	return estimator.num_terms(isquit_func)
468	except:
469	# If we fail, estimate alpha and return the default
470	# number of terms
471	best_alpha, message, elapsed =self.estimate_alpha(self.nfunc)
472	return self.nfunc, best_alpha, "Could not estimate number of terms"
473
474	def estimate_alpha(self, nfunc):
475	"""
476	Returns a reasonable guess for the
477	regularization constant alpha
478
479	:param nfunc: number of terms to use in the expansion.
480
481	:return: alpha, message, elapsed
482
483	where alpha is the estimate for alpha,
484	message is a message for the user,
485	elapsed is the computation time
486	"""
487	import time
488	try:
489	pr = self.clone()
490
491	# T_0 for computation time
492	starttime = time.time()
493	elapsed = 0
494
495	# If the current alpha is zero, try
496	# another value
497	if pr.alpha<=0:
498	pr.alpha = 0.0001
499
500	# Perform inversion to find the largest alpha
501	out, cov = pr.invert(nfunc)
502	elapsed = time.time()-starttime
503	initial_alpha = pr.alpha
504	initial_peaks = pr.get_peaks(out)
505
506	# Try the inversion with the estimated alpha
507	pr.alpha = pr.suggested_alpha
508	out, cov = pr.invert(nfunc)
509
510	npeaks = pr.get_peaks(out)
511	# if more than one peak to start with
512	# just return the estimate
513	if npeaks>1:
514	#message = "Your P(r) is not smooth, please check your inversion parameters"
515	message = None
516	return pr.suggested_alpha, message, elapsed
517	else:
518
519	# Look at smaller values
520	# We assume that for the suggested alpha, we have 1 peak
521	# if not, send a message to change parameters
522	alpha = pr.suggested_alpha
523	best_alpha = pr.suggested_alpha
524	found = False
525	for i in range(10):
526	pr.alpha = (0.33)*(i+1)alpha
527	out, cov = pr.invert(nfunc)
528
529	peaks = pr.get_peaks(out)
530	if peaks>1:
531	found = True
532	break
533	best_alpha = pr.alpha
534
535	# If we didn't find a turning point for alpha and
536	# the initial alpha already had only one peak,
537	# just return that
538	if not found and initial_peaks==1 and initial_alpha<best_alpha:
539	best_alpha = initial_alpha
540
541	# Check whether the size makes sense
542	message=''
543
544	if not found:
545	message = None
546	elif best_alpha>=0.5*pr.suggested_alpha:
547	# best alpha is too big, return a
548	# reasonable value
549	message = "The estimated alpha for your system is too large. "
550	message += "Try increasing your maximum distance."
551
552	return best_alpha, message, elapsed
553
554	except:
555	message = "Invertor.estimate_alpha: %s" % sys.exc_value
556	return 0, message, elapsed
557
558
559	def to_file(self, path, npts=100):
560	"""
561	Save the state to a file that will be readable
562	by SliceView.
563
564	:param path: path of the file to write
565	:param npts: number of P(r) points to be written
566
567	"""
568	file = open(path, 'w')
569	file.write("#d_max=%g\n" % self.d_max)
570	file.write("#nfunc=%g\n" % self.nfunc)
571	file.write("#alpha=%g\n" % self.alpha)
572	file.write("#chi2=%g\n" % self.chi2)
573	file.write("#elapsed=%g\n" % self.elapsed)
574	file.write("#qmin=%s\n" % str(self.q_min))
575	file.write("#qmax=%s\n" % str(self.q_max))
576	file.write("#slit_height=%g\n" % self.slit_height)
577	file.write("#slit_width=%g\n" % self.slit_width)
578	file.write("#background=%g\n" % self.background)
579	if self.has_bck==True:
580	file.write("#has_bck=1\n")
581	else:
582	file.write("#has_bck=0\n")
583	file.write("#alpha_estimate=%g\n" % self.suggested_alpha)
584	if not self.out==None:
585	if len(self.out)==len(self.cov):
586	for i in range(len(self.out)):
587	file.write("#C_%i=%s+-%s\n" % (i, str(self.out[i]), str(self.cov[i][i])))
588	file.write("<r> <Pr> <dPr>\n")
589	r = numpy.arange(0.0, self.d_max, self.d_max/npts)
590
591	for r_i in r:
592	(value, err) = self.pr_err(self.out, self.cov, r_i)
593	file.write("%g %g %g\n" % (r_i, value, err))
594
595	file.close()
596
597
598	def from_file(self, path):
599	"""
600	Load the state of the Invertor from a file,
601	to be able to generate P(r) from a set of
602	parameters.
603
604	:param path: path of the file to load
605
606	"""
607	import os
608	import re
609	if os.path.isfile(path):
610	try:
611	fd = open(path, 'r')
612
613	buff = fd.read()
614	lines = buff.split('\n')
615	for line in lines:
616	if line.startswith('#d_max='):
617	toks = line.split('=')
618	self.d_max = float(toks[1])
619	elif line.startswith('#nfunc='):
620	toks = line.split('=')
621	self.nfunc = int(toks[1])
622	self.out = numpy.zeros(self.nfunc)
623	self.cov = numpy.zeros([self.nfunc, self.nfunc])
624	elif line.startswith('#alpha='):
625	toks = line.split('=')
626	self.alpha = float(toks[1])
627	elif line.startswith('#chi2='):
628	toks = line.split('=')
629	self.chi2 = float(toks[1])
630	elif line.startswith('#elapsed='):
631	toks = line.split('=')
632	self.elapsed = float(toks[1])
633	elif line.startswith('#alpha_estimate='):
634	toks = line.split('=')
635	self.suggested_alpha = float(toks[1])
636	elif line.startswith('#qmin='):
637	toks = line.split('=')
638	try:
639	self.q_min = float(toks[1])
640	except:
641	self.q_min = None
642	elif line.startswith('#qmax='):
643	toks = line.split('=')
644	try:
645	self.q_max = float(toks[1])
646	except:
647	self.q_max = None
648	elif line.startswith('#slit_height='):
649	toks = line.split('=')
650	self.slit_height = float(toks[1])
651	elif line.startswith('#slit_width='):
652	toks = line.split('=')
653	self.slit_width = float(toks[1])
654	elif line.startswith('#background='):
655	toks = line.split('=')
656	self.background = float(toks[1])
657	elif line.startswith('#has_bck='):
658	toks = line.split('=')
659	if int(toks[1])==1:
660	self.has_bck=True
661	else:
662	self.has_bck=False
663
664	# Now read in the parameters
665	elif line.startswith('#C_'):
666	toks = line.split('=')
667	p = re.compile('#C_([0-9]+)')
668	m = p.search(toks[0])
669	toks2 = toks[1].split('+-')
670	i = int(m.group(1))
671	self.out[i] = float(toks2[0])
672
673	self.cov[i][i] = float(toks2[1])
674
675	except:
676	raise RuntimeError, "Invertor.from_file: corrupted file\n%s" % sys.exc_value
677	else:
678	raise RuntimeError, "Invertor.from_file: '%s' is not a file" % str(path)
679
680
681
682
683	if __name__ == "__main__":
684	o = Invertor()
685
686
687
688
689

Note: See TracBrowser for help on using the repository browser.

SasView

source: sasview/pr_inversion/invertor.py @ 3641881

Download in other formats: