def parse_config(filename, defaults={}):
""" Read options for a configuration file.
Parameters
----------
filename : str or file object
The configuration filename or a file object.
defaults : dict
A dictionary with default values for options.
Returns
-------
d : dictionary
The options are returned as a dictionary that can also be
indexed by attribute.
Notes
-----
Ignores blank lines, lines starting with '#', and anything on a
line after a '#'. The parser attempts to convert the values to
int, float or boolean, otherwise they are left as strings.
Sample format::
# this is the file with the line list
lines = lines.dat
x = 20
save = True # save the data
"""
cfg = adict()
cfg.update(defaults)
if isinstance(filename, basestring):
fh = open(filename)
else:
fh = filename
for row in fh:
if not row.strip() or row.lstrip().startswith('#'):
continue
option, value = [r.strip() for r in row.split('#')[0].split('=', 1)]
try:
value = int(value)
except ValueError:
try:
value = float(value)
except ValueError:
if value == 'True':
value = True
elif value == 'False':
value = False
elif value == 'None':
value = None
cfg[option] = value
fh.close()
return cfg
def calc_Wr(i0, i1, wa, tr, ew=None, ewer=None, fl=None, er=None, co=None,
cohi=0.02, colo=0.02):
""" Find the rest equivalent width of a feature, and column
density assuming optically thin.
Parameters
----------
i0, i1 : int
Start and end indices of feature (inclusive).
wa : array of floats, shape (N,)
Observed wavelengths.
tr : atom.dat entry
Transition entry from an atom.dat array read by `readatom()`.
ew : array of floats, shape (N,), optional
Equivalent width per pixel.
ewer : array of floats, shape (N,), optional
Equivalent width 1 sigma error per pixel.
with attributes wav (rest wavelength) and osc (oscillator strength).
fl : array of floats, shape (N,), optional
Observed flux.
er : array of floats, shape (N,), optional
Observed flux 1 sigma error.
co : array of floats, shape (N,), optional
Observed continuum.
cohi : float (0.02)
When calculating one sigma upper error and detection limit,
increase the continuum by this fractional amount. Only used if
fl, er and co are also given.
colo : float (0.02)
When calculating one sigma lower error decrease the continuum by
this fractional amount. Only used if fl, er and co are also
given.
Returns
-------
A dictionary with keys:
======== =========================================================
logN 1 sigma low val, value, 1 sigma upper val
Ndetlim log N 5 sigma upper limit
Wr Rest equivalent width in same units as wa
Wre 1 sigma error on rest equivalent width
zp1 1 + redshift
ngoodpix number of good pixels contributing to the measurements
Nmult multiplier to get from equivalent width to column density
======== =========================================================
"""
wa1 = wa[i0:i1+1]
if ew is None:
wedge = find_wa_edges(wa1)
dw = wedge[1:] - wedge[:-1]
ew1 = dw * (1 - fl[i0:i1+1] / co[i0:i1+1])
ewer1 = dw * er[i0:i1+1] / co[i0:i1+1]
c = (1 + cohi) * co[i0:i1+1]
ew1hi = dw * (1 - fl[i0:i1+1] / c)
ewer1hi = dw * er[i0:i1+1] / c
c = (1 - colo) * co[i0:i1+1]
ew1lo = dw * (1 - fl[i0:i1+1] / c)
ewer1lo = dw * er[i0:i1+1] / c
else:
ew1 = np.array(ew[i0:i1+1])
ewer1 = np.array(ewer[i0:i1+1])
# interpolate over bad values
good = ~np.isnan(ew1) & (ewer1 > 0)
if not good.all():
ew1[~good] = np.interp(wa1[~good], wa1[good], ew1[good])
ewer1[~good] = np.interp(wa1[~good], wa1[good], ewer1[good])
if fl is not None:
ew1hi[~good] = np.interp(wa1[~good], wa1[good], ew1hi[good])
ewer1hi[~good] = np.interp(wa1[~good], wa1[good], ewer1hi[good])
ew1lo[~good] = np.interp(wa1[~good], wa1[good], ew1lo[good])
ewer1lo[~good] = np.interp(wa1[~good], wa1[good], ewer1lo[good])
W = ew1.sum()
We = sqrt((ewer1**2).sum())
if fl is not None:
Whi = ew1hi.sum()
Wehi = sqrt((ewer1hi**2).sum())
Wlo = ew1lo.sum()
Welo = sqrt((ewer1lo**2).sum())
zp1 = 0.5*(wa1[0] + wa1[-1]) / tr['wa']
Wr = W / zp1
Wre = We / zp1
if fl is not None:
Wrhi = Whi / zp1
Wrehi = Wehi / zp1
Wrlo = Wlo / zp1
Wrelo = Welo / zp1
# Assume we are on the linear part of curve of growth (will be an
# underestimate if saturated)
Nmult = 1.13e20 / (tr['osc'] * tr['wa']**2)
# 5 sigma detection limit
detlim = np.log10( Nmult * 5*Wre )
c = np.log10(Nmult * Wr)
if fl is not None:
chi = np.log10( Nmult * (Wrhi + Wrehi) )
clo = np.log10( Nmult * (Wrlo - Wrelo) )
else:
chi = np.log10( Nmult * (Wr + Wre) )
clo = np.log10( Nmult * (Wr - Wre) )
return adict(logN=(clo,c,chi), Ndetlim=detlim, Wr=Wr, Wre=Wre, zp1=zp1,
ngoodpix=good.sum(), Nmult=Nmult)