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我正在爲基於scipy的optimize.leastsq的2D數據編寫一個自動曲線擬合例程，它可以工作。然而，當添加很多曲線時，我會得到非物理結果（例如負振幅）。根據MINUIT的Python參數轉換
我發現此帖子Scipy: bounds for fitting parameter(s) when using optimize.leastsq並試圖根據Cern的Minuit使用參數轉換。在上面提到的問題中，有人提供了一些鏈接到一些python代碼。
code.google.com/p/nmrglue/source/browse/trunk/nmrglue/analysis/leastsqbound.py
我寫這個最小工作示例（擴展代碼）
"""
http://code.google.com/p/nmrglue/source/browse/trunk/nmrglue/analysis/leastsqbound.py
Constrained multivariate Levenberg-Marquardt optimization
"""
from scipy.optimize import leastsq
import numpy as np
import matplotlib.pyplot as plt #new
def internal2external_grad(xi, bounds):
"""
Calculate the internal to external gradiant
Calculates the partial of external over internal
"""
ge = np.empty_like(xi)
for i, (v, bound) in enumerate(zip(xi, bounds)):
a = bound[0] # minimum
b = bound[1] # maximum
if a == None and b == None: # No constraints
ge[i] = 1.0
elif b == None: # only min
ge[i] = v/np.sqrt(v ** 2 + 1)
elif a == None: # only max
ge[i] = -v/np.sqrt(v ** 2 + 1)
else: # both min and max
ge[i] = (b - a) * np.cos(v)/2.
return ge
def i2e_cov_x(xi, bounds, cov_x):
grad = internal2external_grad(xi, bounds)
grad = grad = np.atleast_2d(grad)
return np.dot(grad.T, grad) * cov_x
def internal2external(xi, bounds):
""" Convert a series of internal variables to external variables"""
xe = np.empty_like(xi)
for i, (v, bound) in enumerate(zip(xi, bounds)):
a = bound[0] # minimum
b = bound[1] # maximum
if a == None and b == None: # No constraints
xe[i] = v
elif b == None: # only min
xe[i] = a - 1. + np.sqrt(v ** 2. + 1.)
elif a == None: # only max
xe[i] = b + 1. - np.sqrt(v ** 2. + 1.)
else: # both min and max
xe[i] = a + ((b - a)/2.) * (np.sin(v) + 1.)
return xe
def external2internal(xe, bounds):
""" Convert a series of external variables to internal variables"""
xi = np.empty_like(xe)
for i, (v, bound) in enumerate(zip(xe, bounds)):
a = bound[0] # minimum
b = bound[1] # maximum
if a == None and b == None: # No constraints
xi[i] = v
elif b == None: # only min
xi[i] = np.sqrt((v - a + 1.) ** 2. - 1)
elif a == None: # only max
xi[i] = np.sqrt((b - v + 1.) ** 2. - 1)
else: # both min and max
xi[i] = np.arcsin((2.*(v - a)/(b - a)) - 1.)
return xi
def err(p, bounds, efunc, args):
pe = internal2external(p, bounds) # convert to external variables
return efunc(pe, *args)
def calc_cov_x(infodic, p):
"""
Calculate cov_x from fjac, ipvt and p as is done in leastsq
"""
fjac = infodic['fjac']
ipvt = infodic['ipvt']
n = len(p)
# adapted from leastsq function in scipy/optimize/minpack.py
perm = np.take(np.eye(n), ipvt - 1, 0)
r = np.triu(np.transpose(fjac)[:n, :])
R = np.dot(r, perm)
try:
cov_x = np.linalg.inv(np.dot(np.transpose(R), R))
except LinAlgError:
cov_x = None
return cov_x
def leastsqbound(func, x0, bounds, args =(), **kw):
"""
Constrained multivariant Levenberg-Marquard optimization
Minimize the sum of squares of a given function using the
Levenberg-Marquard algorithm. Contraints on parameters are inforced using
variable transformations as described in the MINUIT User's Guide by
Fred James and Matthias Winkler.
Parameters:
* func functions to call for optimization.
* x0 Starting estimate for the minimization.
* bounds (min,max) pair for each element of x, defining the bounds on
that parameter. Use None for one of min or max when there is
no bound in that direction.
* args Any extra arguments to func are places in this tuple.
Returns: (x,{cov_x,infodict,mesg},ier)
Return is described in the scipy.optimize.leastsq function. x and con_v
are corrected to take into account the parameter transformation, infodic
is not corrected.
Additional keyword arguments are passed directly to the
scipy.optimize.leastsq algorithm.
"""
# check for full output
if "full_output" in kw and kw["full_output"]:
full = True
else:
full = False
# convert x0 to internal variables
i0 = external2internal(x0, bounds)
# perfrom unconstrained optimization using internal variables
r = leastsq(err, i0, args = (bounds, func, args), **kw)
# unpack return convert to external variables and return
if full:
xi, cov_xi, infodic, mesg, ier = r
xe = internal2external(xi, bounds)
cov_xe = i2e_cov_x(xi, bounds, cov_xi)
# XXX correct infodic 'fjac','ipvt', and 'qtf'
return xe, cov_xe, infodic, mesg, ier
else:
xi, ier = r
xe = internal2external(xi, bounds)
return xe, ier
# new below
def _evaluate(x, p):
'''
Linear plus Lorentzian curve
p = list with three parameters ([a, b, I, Pos, FWHM])
'''
return p[0] + p[1] * x + p[2]/(1 + np.power((x - p[3])/(p[4]/2), 2))
def residuals(p, y, x):
err = _evaluate(x, p) - y
return err
if __name__ == '__main__':
data = np.loadtxt('constraint.dat') # read data
p0 = [5000., 0., 500., 2450., 3] #Start values for a, b, I, Pos, FWHM
constraints = [(4000., None), (-50., 20.), (0., 2000.), (2400., 2451.), (None, None)]
p, res = leastsqbound(residuals, p0, constraints, args = (data[:, 1], data[:, 0]), maxfev = 20000)
print p, res
plt.plot(data[:, 0], data[:, 1]) # plot data
plt.plot(data[:, 0], _evaluate(data[:, 0], p0)) # plot start values
plt.plot(data[:, 0], _evaluate(data[:, 0], p)) # plot fit values
plt.show()
那情節輸出，其中綠色是啓動條件和紅色的擬合結果： 
這是正確的用法？ External2internal轉換隻是在邊界外拋出一個nan。 leastsq似乎能夠處理這個問題？
我上傳了擬合數據here。只需粘貼到名爲constraint.dat的文本文件中即可。
謝謝你指出這一點。我之前沒有找到任何有關mpfit的參考，它看起來正是我試圖達到的目標。但是，一個最小的工作例子會是怎樣的呢？用法與scipy的leastsq不同。看起來x和y值沒有通過，而是參考？mpfit.py中的例子也不起作用。 – user334287
下面是一個例子，它絕對有效： http://code.google.com/p/astrolibpy/source/browse/mpfit/tests/test_mpfit.py –
我用你鏈接的testfile的第一個例子來獲取解決方案在運行。我最初有點困惑，因爲他們使用起始值_p0 = [1,1] _但在參數字典_parinfo_中他們使用3.2和1.78。另外，_p0_實際上在通話中不是必需的。 – user334287