def _polyarea3D(xyz):
x, y, z = asplit(xyz)
RY = np.sqrt((x[0] - x[1])**2 + (y[0] - y[1])**2 + (z[0] - z[1])**2)
YG = np.sqrt((x[1] - x[2])**2 + (y[1] - y[2])**2 + (z[1] - z[2])**2)
GR = np.sqrt((x[2] - x[0])**2 + (y[2] - y[0])**2 + (z[2] - z[0])**2)
RB = np.sqrt((x[0] - x[3])**2 + (y[0] - y[3])**2 + (z[0] - z[3])**2)
BG = np.sqrt((x[2] - x[3])**2 + (y[2] - y[3])**2 + (z[2] - z[3])**2)
S1 = (RY + YG + GR) / 2
S2 = (RB + BG + GR) / 2
GA1 = np.sqrt(S1 * (S1 - RY) * (S1 - YG) * (S1 - GR))
GA2 = np.sqrt(S2 * (S2 - RB) * (S2 - BG) * (S2 - GR))
GA = GA1 + GA2
return GA
def smet2017_D(xyzw, Dmax=None):
"""
Calculate the degree of adaptation based on chromaticity following
Smet et al. (2017)
Args:
:xyzw:
| ndarray with white point data (CIE 1964 10° XYZs!!)
:Dmax:
| None or float, optional
| Defaults to 0.6539 (max D obtained under experimental conditions,
| but probably too low due to dark surround leading to incomplete
| chromatic adaptation even for neutral illuminants
| resulting in background luminance (fov~50°) of 760 cd/m²))
Returns:
:D:
| ndarray with degrees of adaptation
References:
1. `Smet, K.A.G.*, Zhai, Q., Luo, M.R., Hanselaer, P., (2017),
Study of chromatic adaptation using memory color matches,
Part II: colored illuminants,
Opt. Express, 25(7), pp. 8350-8365.
<https://www.osapublishing.org/oe/abstract.cfm?uri=oe-25-7-8350&origin=search)>`_
"""
# Convert xyzw to log-compressed Macleod_Boyton coordinates:
Vl, rl, bl = asplit(
np.log(xyz_to_Vrb_mb(xyzw, M=_MCATS['hpe']))
) # force use of HPE matrix (which was the one used when deriving the model parameters!!)
# apply Dmodel (technically only for cieobs = '1964_10')
pD = (1.0e7) * np.array([
0.021081326530436, 4.751255762876845, -0.000000071025181,
-0.000000063627042, -0.146952821492957, 3.117390441655821
]) #D model parameters for gaussian model in log(MB)-space (july 2016)
if Dmax is None:
Dmax = 0.6539 # max D obtained under experimental conditions (probably too low due to dark surround leading to incomplete chromatic adaptation even for neutral illuminants resulting in background luminance (fov~50°) of 760 cd/m²)
return Dmax * math.bvgpdf(x=rl,
y=bl,
mu=pD[2:4],
sigmainv=np.linalg.inv(
np.array([[pD[0], pD[4]], [pD[4], pD[1]]
])))**pD[5]
def spd_to_mcri(SPD, D = 0.9, E = None, Yb = 20.0, out = 'Rm', wl = None):
"""
Calculates the MCRI or Memory Color Rendition Index, Rm
Args:
:SPD:
| ndarray with spectral data (can be multiple SPDs,
| first axis are the wavelengths)
:D:
| 0.9, optional
| Degree of adaptation.
:E:
| None, optional
| Illuminance in lux
| (used to calculate La = (Yb/100)*(E/pi) to then calculate D
| following the 'cat02' model).
| If None: the degree is determined by :D:
| If (:E: is not None) & (:Yb: is None): :E: is assumed to contain
| the adapting field luminance La (cd/m²).
:Yb:
| 20.0, optional
| Luminance factor of background. (used when calculating La from E)
| If None, E contains La (cd/m²).
:out:
| 'Rm' or str, optional
| Specifies requested output (e.g. 'Rm,Rmi,cct,duv')
:wl:
| None, optional
| Wavelengths (or [start, end, spacing]) to interpolate the SPDs to.
| None: default to no interpolation
Returns:
:returns:
| float or ndarray with MCRI Rm for :out: 'Rm'
| Other output is also possible by changing the :out: str value.
References:
1. `K.A.G. Smet, W.R. Ryckaert, M.R. Pointer, G. Deconinck, P. Hanselaer,(2012)
“A memory colour quality metric for white light sources,”
Energy Build., vol. 49, no. C, pp. 216–225.
<http://www.sciencedirect.com/science/article/pii/S0378778812000837>`_
"""
SPD = np2d(SPD)
if wl is not None:
SPD = spd(data = SPD, interpolation = _S_INTERP_TYPE, kind = 'np', wl = wl)
# unpack metric default values:
avg, catf, cieobs, cri_specific_pars, cspace, ref_type, rg_pars, sampleset, scale = [_MCRI_DEFAULTS[x] for x in sorted(_MCRI_DEFAULTS.keys())]
similarity_ai = cri_specific_pars['similarity_ai']
Mxyz2lms = cspace['Mxyz2lms']
scale_fcn = scale['fcn']
scale_factor = scale['cfactor']
sampleset = eval(sampleset)
# A. calculate xyz:
xyzti, xyztw = spd_to_xyz(SPD, cieobs = cieobs['xyz'], rfl = sampleset, out = 2)
if 'cct' in out.split(','):
cct, duv = xyz_to_cct(xyztw, cieobs = cieobs['cct'], out = 'cct,duv',mode = 'lut')
# B. perform chromatic adaptation to adopted whitepoint of ipt color space, i.e. D65:
if catf is not None:
Dtype_cat, F, Yb_cat, catmode_cat, cattype_cat, mcat_cat, xyzw_cat = [catf[x] for x in sorted(catf.keys())]
# calculate degree of adaptationn D:
if E is not None:
if Yb is not None:
La = (Yb/100.0)*(E/np.pi)
else:
La = E
D = cat.get_degree_of_adaptation(Dtype = Dtype_cat, F = F, La = La)
else:
Dtype_cat = None # direct input of D
if (E is None) and (D is None):
D = 1.0 # set degree of adaptation to 1 !
if D > 1.0: D = 1.0
if D < 0.6: D = 0.6 # put a limit on the lowest D
# apply cat:
xyzti = cat.apply(xyzti, cattype = cattype_cat, catmode = catmode_cat, xyzw1 = xyztw,xyzw0 = None, xyzw2 = xyzw_cat, D = D, mcat = [mcat_cat], Dtype = Dtype_cat)
xyztw = cat.apply(xyztw, cattype = cattype_cat, catmode = catmode_cat, xyzw1 = xyztw,xyzw0 = None, xyzw2 = xyzw_cat, D = D, mcat = [mcat_cat], Dtype = Dtype_cat)
# C. convert xyz to ipt and split:
ipt = xyz_to_ipt(xyzti, cieobs = cieobs['xyz'], M = Mxyz2lms) #input matrix as published in Smet et al. 2012, Energy and Buildings
I,P,T = asplit(ipt)
# D. calculate specific (hue dependent) similarity indicators, Si:
if len(xyzti.shape) == 3:
ai = np.expand_dims(similarity_ai, axis = 1)
else:
ai = similarity_ai
a1,a2,a3,a4,a5 = asplit(ai)
mahalanobis_d2 = (a3*np.power((P - a1),2.0) + a4*np.power((T - a2),2.0) + 2.0*a5*(P-a1)*(T-a2))
if (len(mahalanobis_d2.shape)==3) & (mahalanobis_d2.shape[-1]==1):
mahalanobis_d2 = mahalanobis_d2[:,:,0].T
Si = np.exp(-0.5*mahalanobis_d2)
# E. calculate general similarity indicator, Sa:
Sa = avg(Si, axis = 0,keepdims = True)
# F. rescale similarity indicators (Si, Sa) with a 0-1 scale to memory color rendition indices (Rmi, Rm) with a 0 - 100 scale:
Rmi = scale_fcn(np.log(Si),scale_factor = scale_factor)
Rm = np2d(scale_fcn(np.log(Sa),scale_factor = scale_factor))
# G. calculate Rg (polyarea of test / polyarea of memory colours):
if 'Rg' in out.split(','):
I = I[...,None] #broadcast_shape(I, target_shape = None,expand_2d_to_3d = 0)
a1 = a1[:,None]*np.ones(I.shape)#broadcast_shape(a1, target_shape = None,expand_2d_to_3d = 0)
a2 = a2[:,None]*np.ones(I.shape) #broadcast_shape(a2, target_shape = None,expand_2d_to_3d = 0)
a12 = np.concatenate((a1,a2),axis=2) #broadcast_shape(np.hstack((a1,a2)), target_shape = ipt.shape,expand_2d_to_3d = 0)
ipt_mc = np.concatenate((I,a12),axis=2)
nhbins, normalize_gamut, normalized_chroma_ref, start_hue = [rg_pars[x] for x in sorted(rg_pars.keys())]
hue_bin_data = _get_hue_bin_data(ipt, ipt_mc,
start_hue = start_hue, nhbins = nhbins,
normalized_chroma_ref = normalized_chroma_ref)
Rg = _hue_bin_data_to_rg(hue_bin_data)
if (out != 'Rm'):
return eval(out)
else:
return Rm
def mahalanobis2(x, y = None, z = None, mu = None, sigmainv = None):
"""
Evaluate the squared mahalanobis distance
Args:
:x:
| scalar or list or ndarray (.ndim = 1 or 2) with x(y)-coordinates
at which to evaluate the mahalanobis distance squared.
:y:
| None or scalar or list or ndarray (.ndim = 1) with y-coordinates
at which to evaluate the mahalanobis distance squared, optional.
| If :y: is None, :x: should be a 2d array.
:z:
| None or scalar or list or ndarray (.ndim = 1) with z-coordinates
at which to evaluate the mahalanobis distance squared, optional.
| If :z: is None & :y: is None, then :x: should be a 2d array.
:mu:
| None or ndarray (.ndim = 1) with center coordinates of the
mahalanobis ellipse, optional.
| None defaults to zeros(2) or zeros(3).
:sigmainv:
| None or ndarray with 'inverse covariance matrix', optional
| Determines the shape and orientation of the PD.
| None default to np.eye(2) or eye(3).
Returns:
:returns:
| ndarray with magnitude of mahalanobis2(x,y[,z])
"""
if (y is None) & (z is None):
p = x.shape[-1]
elif (z is None):
p = x.shape[-1] if (y is None) else 2
elif (z is not None):
p = 3 if (y is not None) else 2
if mu is None:
mu = np.zeros(p)
if sigmainv is None:
sigmainv = np.eye(p)
x = np2d(x)
mu = np2d(mu)
if (y is None) & (z is None):
x = x - mu
if p == 2:
x, y = asplit(x)
elif p==3:
x, y, z = asplit(x)
elif (z is None):
if y is None:
x = x - mu
x, y = asplit(x)
else:
x = x - mu[...,0] # center data on mu
y = np2d(y) - mu[...,1] # center data on mu
elif (z is not None):
if (y is not None):
x = x - mu[0] # center data on mu
y = np2d(y) - mu[...,1] # center data on mu
z = np2d(z) - mu[...,2] # center data on mu
else:
x = x - mu[...,0] # center data on mu
y = np2d(z) - mu[...,1] # center data on mu
if p == 2:
return (sigmainv[0,0] * (x**2.0) + sigmainv[1,1] * (y**2.0) + 2.0*sigmainv[0,1]*(x*y))
else:
return (sigmainv[0,0] * (x**2.0) + sigmainv[1,1] * (y**2.0) + 2.0*sigmainv[0,1]*(x*y) +
sigmainv[2,2] * (z**2.0) + 2.0*sigmainv[0,2]*(x*z) + 2.0*sigmainv[1,2]*(y*z))
def plot_chromaticity_diagram_colors(diagram_samples = 256, diagram_opacity = 1.0, diagram_lightness = 0.25,\
cieobs = _CIEOBS, cspace = 'Yxy', cspace_pars = {},\
show = True, axh = None,\
show_grid = False, label_fontname = 'Times New Roman', label_fontsize = 12,\
**kwargs):
"""
Plot the chromaticity diagram colors.
Args:
:diagram_samples:
| 256, optional
| Sampling resolution of color space.
:diagram_opacity:
| 1.0, optional
| Sets opacity of chromaticity diagram
:diagram_lightness:
| 0.25, optional
| Sets lightness of chromaticity diagram
:axh:
| None or axes handle, optional
| Determines axes to plot data in.
| None: make new figure.
:show:
| True or False, optional
| Invoke matplotlib.pyplot.show() right after plotting
:cieobs:
| luxpy._CIEOBS or str, optional
| Determines CMF set to calculate spectrum locus or other.
:cspace:
| luxpy._CSPACE or str, optional
| Determines color space / chromaticity diagram to plot data in.
| Note that data is expected to be in specified :cspace:
:cspace_pars:
| {} or dict, optional
| Dict with parameters required by color space specified in :cspace:
| (for use with luxpy.colortf())
:show_grid:
| False, optional
| Show grid (True) or not (False)
:label_fontname:
| 'Times New Roman', optional
| Sets font type of axis labels.
:label_fontsize:
| 12, optional
| Sets font size of axis labels.
:kwargs:
| additional keyword arguments for use with matplotlib.pyplot.
Returns:
"""
if isinstance(cieobs, str):
SL = _CMF[cieobs]['bar'][1:4].T
else:
SL = cieobs[1:4].T
SL = 100.0 * SL / (SL[:, 1, None] + _EPS)
SL = SL[SL.sum(axis=1) >
0, :] # avoid div by zero in xyz-to-Yxy conversion
SL = colortf(SL, tf=cspace, tfa0=cspace_pars)
plambdamax = SL[:, 1].argmax()
SL = np.vstack(
(SL[:(plambdamax + 1), :], SL[0])
) # add lowest wavelength data and go to max of gamut in x (there is a reversal for some cmf set wavelengths >~700 nm!)
Y, x, y = asplit(SL)
SL = np.vstack((x, y)).T
# create grid for conversion to srgb
offset = _EPS
min_x = min(offset, x.min())
max_x = max(1, x.max())
min_y = min(offset, y.min())
max_y = max(1, y.max())
ii, jj = np.meshgrid(
np.linspace(min_x - offset, max_x + offset, int(diagram_samples)),
np.linspace(max_y + offset, min_y - offset, int(diagram_samples)))
ij = np.dstack((ii, jj))
ij[ij == 0] = offset
ij2D = ij.reshape((diagram_samples**2, 2))
ij2D = np.hstack((diagram_lightness * 100 * np.ones(
(ij2D.shape[0], 1)), ij2D))
xyz = colortf(ij2D, tf=cspace + '>xyz', tfa0=cspace_pars)
xyz[xyz < 0] = 0
xyz[np.isinf(xyz.sum(axis=1)), :] = np.nan
xyz[np.isnan(xyz.sum(axis=1)), :] = offset
srgb = xyz_to_srgb(xyz)
srgb = srgb / srgb.max()
srgb = srgb.reshape((diagram_samples, diagram_samples, 3))
if show == True:
if axh is None:
fig = plt.figure()
axh = fig.add_subplot(111)
polygon = Polygon(SL, facecolor='none', edgecolor='none')
axh.add_patch(polygon)
image = axh.imshow(srgb,
interpolation='bilinear',
extent=(min_x, max_x, min_y - 0.05, max_y),
clip_path=None,
alpha=diagram_opacity)
image.set_clip_path(polygon)
axh.plot(x, y, color='darkgray')
if (cspace == 'Yxy') & (isinstance(cieobs, str)):
axh.set_xlim([0, 1])
axh.set_ylim([0, 1])
elif (cspace == 'Yuv') & (isinstance(cieobs, str)):
axh.set_xlim([0, 0.6])
axh.set_ylim([0, 0.6])
if (cspace is not None):
xlabel = _CSPACE_AXES[cspace][1]
ylabel = _CSPACE_AXES[cspace][2]
if (label_fontname is not None) & (label_fontsize is not None):
axh.set_xlabel(xlabel,
fontname=label_fontname,
fontsize=label_fontsize)
axh.set_ylabel(ylabel,
fontname=label_fontname,
fontsize=label_fontsize)
if show_grid == True:
axh.grid(True)
#plt.show()
return axh
else:
return None
def plotSL(cieobs =_CIEOBS, cspace = _CSPACE, DL = False, BBL = True, D65 = False,\
EEW = False, cctlabels = False, axh = None, show = True,\
cspace_pars = {}, formatstr = 'k-',\
diagram_colors = False, diagram_samples = 100, diagram_opacity = 1.0,\
diagram_lightness = 0.25,\
**kwargs):
"""
Plot spectrum locus for cieobs in cspace.
Args:
:DL:
| True or False, optional
| True plots Daylight Locus as well.
:BBL:
| True or False, optional
| True plots BlackBody Locus as well.
:D65:
| False or True, optional
| True plots D65 chromaticity as well.
:EEW:
| False or True, optional
| True plots Equi-Energy-White chromaticity as well.
:cctlabels:
| False or True, optional
| Add cct text labels at various points along the blackbody locus.
:axh:
| None or axes handle, optional
| Determines axes to plot data in.
| None: make new figure.
:show:
| True or False, optional
| Invoke matplotlib.pyplot.show() right after plotting
:cieobs:
| luxpy._CIEOBS or str, optional
| Determines CMF set to calculate spectrum locus or other.
:cspace:
| luxpy._CSPACE or str, optional
| Determines color space / chromaticity diagram to plot data in.
| Note that data is expected to be in specified :cspace:
:formatstr:
| 'k-' or str, optional
| Format str for plotting (see ?matplotlib.pyplot.plot)
:cspace_pars:
| {} or dict, optional
| Dict with parameters required by color space specified in :cspace:
| (for use with luxpy.colortf())
:diagram_colors:
| False, optional
| True: plot colored chromaticity diagram.
:diagram_samples:
| 256, optional
| Sampling resolution of color space.
:diagram_opacity:
| 1.0, optional
| Sets opacity of chromaticity diagram
:diagram_lightness:
| 0.25, optional
| Sets lightness of chromaticity diagram
:kwargs:
| additional keyword arguments for use with matplotlib.pyplot.
Returns:
:returns:
| None (:show: == True)
| or
| handle to current axes (:show: == False)
"""
if isinstance(cieobs, str):
SL = _CMF[cieobs]['bar'][1:4].T
else:
SL = cieobs[1:4].T
SL = 100.0 * SL / (SL[:, 1, None] + _EPS)
SL = SL[SL.sum(axis=1) >
0, :] # avoid div by zero in xyz-to-Yxy conversion
SL = colortf(SL, tf=cspace, tfa0=cspace_pars)
plambdamax = SL[:, 1].argmax()
SL = np.vstack(
(SL[:(plambdamax + 1), :], SL[0])
) # add lowest wavelength data and go to max of gamut in x (there is a reversal for some cmf set wavelengths >~700 nm!)
Y, x, y = asplit(SL)
showcopy = show
if np.any([DL, BBL, D65, EEW]):
show = False
if diagram_colors == True:
axh_ = plot_chromaticity_diagram_colors(axh = axh, show = diagram_colors, cspace = cspace, cieobs = cieobs,\
cspace_pars = cspace_pars,\
diagram_samples = diagram_samples,\
diagram_opacity = diagram_opacity,\
diagram_lightness = diagram_lightness,\
label_fontname = None, label_fontsize = None)
else:
axh_ = axh
axh_ = plot_color_data(x,
y,
axh=axh_,
cieobs=cieobs,
cspace=cspace,
show=show,
formatstr=formatstr,
**kwargs)
if DL == True:
if 'label' in kwargs.keys(): # avoid label also being used for DL
kwargs.pop('label')
plotDL(ccts=None,
cieobs=cieobs,
cspace=cspace,
axh=axh_,
show=show,
cspace_pars=cspace_pars,
formatstr='k:',
**kwargs)
if BBL == True:
if 'label' in kwargs.keys(): # avoid label also being used for BB
kwargs.pop('label')
plotBB(ccts=None,
cieobs=cieobs,
cspace=cspace,
axh=axh_,
show=show,
cspace_pars=cspace_pars,
cctlabels=cctlabels,
formatstr='k-.',
**kwargs)
if D65 == True:
YxyD65 = colortf(spd_to_xyz(_CIE_ILLUMINANTS['D65'], cieobs=cieobs),
tf=cspace,
tfa0=cspace_pars)
axh.plot(YxyD65[..., 1], YxyD65[..., 2], 'bo')
if EEW == True:
YxyEEW = colortf(spd_to_xyz(_CIE_ILLUMINANTS['E'], cieobs=cieobs),
tf=cspace,
tfa0=cspace_pars)
axh.plot(YxyEEW[..., 1], YxyEEW[..., 2], 'ko')
if showcopy == False:
return axh_
else:
plt.show()
def plotBB(ccts=None,
cieobs=_CIEOBS,
cspace=_CSPACE,
axh=None,
cctlabels=True,
show=True,
cspace_pars={},
formatstr='k-',
**kwargs):
"""
Plot blackbody locus.
Args:
:ccts:
| None or list[float], optional
| None defaults to [1000 to 1e19 K].
| Range:
| [1000,1500,2000,2500,3000,3500,4000,5000,6000,8000,10000]
| + [15000 K to 1e19 K] in 100 steps on a log10 scale
:cctlabels:
| True or False, optional
| Add cct text labels at various points along the blackbody locus.
:axh:
| None or axes handle, optional
| Determines axes to plot data in.
| None: make new figure.
:show:
| True or False, optional
| Invoke matplotlib.pyplot.show() right after plotting
:cieobs:
| luxpy._CIEOBS or str, optional
| Determines CMF set to calculate spectrum locus or other.
:cspace:
| luxpy._CSPACE or str, optional
| Determines color space / chromaticity diagram to plot data in.
| Note that data is expected to be in specified :cspace:
:formatstr:
| 'k-' or str, optional
| Format str for plotting (see ?matplotlib.pyplot.plot)
:cspace_pars:
| {} or dict, optional
| Dict with parameters required by color space specified in :cspace:
| (for use with luxpy.colortf())
:kwargs:
| additional keyword arguments for use with matplotlib.pyplot.
Returns:
:returns:
| None (:show: == True)
| or
| handle to current axes (:show: == False)
"""
if ccts is None:
ccts1 = np.array([
1000.0, 1500.0, 2000.0, 2500.0, 3000.0, 3500.0, 4000.0, 5000.0,
6000.0, 8000.0, 10000.0
])
ccts2 = 10**np.linspace(np.log10(15000.0), np.log10(10.0**19.0), 100)
ccts = np.hstack((ccts1, ccts2))
else:
ccts1 = None
BB = cri_ref(ccts, ref_type='BB')
xyz = spd_to_xyz(BB, cieobs=cieobs)
Yxy = colortf(xyz, tf=cspace, tfa0=cspace_pars)
Y, x, y = asplit(Yxy)
axh = plot_color_data(x,
y,
axh=axh,
cieobs=cieobs,
cspace=cspace,
show=show,
formatstr=formatstr,
**kwargs)
if (cctlabels == True) & (ccts1 is not None):
for i in range(ccts1.shape[0]):
if ccts1[i] >= 3000.0:
if i % 2 == 0.0:
axh.plot(x[i], y[i], 'k+', color='0.5')
axh.text(x[i] * 1.05,
y[i] * 0.95,
'{:1.0f}K'.format(ccts1[i]),
color='0.5')
axh.plot(x[-1], y[-1], 'k+', color='0.5')
axh.text(x[-1] * 1.05,
y[-1] * 0.95,
'{:1.0e}K'.format(ccts[-1]),
color='0.5')
if show == False:
return axh
def plotDL(ccts = None, cieobs =_CIEOBS, cspace = _CSPACE, axh = None, \
show = True, force_daylight_below4000K = False, cspace_pars = {}, \
formatstr = 'k-', **kwargs):
"""
Plot daylight locus.
Args:
:ccts:
| None or list[float], optional
| None defaults to [4000 K to 1e19 K] in 100 steps on a log10 scale.
:force_daylight_below4000K:
| False or True, optional
| CIE daylight phases are not defined below 4000 K.
| If True plot anyway.
:axh:
| None or axes handle, optional
| Determines axes to plot data in.
| None: make new figure.
:show:
| True or False, optional
| Invoke matplotlib.pyplot.show() right after plotting
:cieobs:
| luxpy._CIEOBS or str, optional
| Determines CMF set to calculate spectrum locus or other.
:cspace:
| luxpy._CSPACE or str, optional
| Determines color space / chromaticity diagram to plot data in.
| Note that data is expected to be in specified :cspace:
:formatstr:
| 'k-' or str, optional
| Format str for plotting (see ?matplotlib.pyplot.plot)
:cspace_pars:
| {} or dict, optional
| Dict with parameters required by color space specified in :cspace:
| (for use with luxpy.colortf())
:kwargs:
| additional keyword arguments for use with matplotlib.pyplot.
Returns:
:returns:
| None (:show: == True)
| or
| handle to current axes (:show: == False)
"""
if ccts is None:
ccts = 10**np.linspace(np.log10(4000.0), np.log10(10.0**19.0), 100)
xD, yD = daylightlocus(ccts,
cieobs=cieobs,
force_daylight_below4000K=force_daylight_below4000K)
Y = 100 * np.ones(xD.shape)
DL = Yxy_to_xyz(np.vstack((Y, xD, yD)).T)
DL = colortf(DL, tf=cspace, tfa0=cspace_pars)
Y, x, y = asplit(DL)
axh = plot_color_data(x,
y,
axh=axh,
cieobs=cieobs,
cspace=cspace,
show=show,
formatstr=formatstr,
**kwargs)
if show == False:
return axh
def xyz_to_Ydlep(xyz,
cieobs=_CIEOBS,
xyzw=_COLORTF_DEFAULT_WHITE_POINT,
flip_axes=False,
SL_max_lambda=None,
**kwargs):
"""
Convert XYZ tristimulus values to Y, dominant (complementary) wavelength
and excitation purity.
Args:
:xyz:
| ndarray with tristimulus values
:xyzw:
| None or ndarray with tristimulus values of a single (!) native white point, optional
| None defaults to xyz of CIE D65 using the :cieobs: observer.
:cieobs:
| luxpy._CIEOBS, optional
| CMF set to use when calculating spectrum locus coordinates.
:flip_axes:
| False, optional
| If True: flip axis 0 and axis 1 in Ydelep to increase speed of loop in function.
| (single xyzw with is not flipped!)
:SL_max_lambda:
| None or float, optional
| Maximum wavelength of spectrum locus before it turns back on itelf in the high wavelength range (~700 nm)
Returns:
:Ydlep:
| ndarray with Y, dominant (complementary) wavelength
| and excitation purity
"""
xyz3 = np3d(xyz).copy().astype(np.float)
# flip axis so that shortest dim is on axis0 (save time in looping):
if (xyz3.shape[0] < xyz3.shape[1]) & (flip_axes == True):
axes12flipped = True
xyz3 = xyz3.transpose((1, 0, 2))
else:
axes12flipped = False
# convert xyz to Yxy:
Yxy = xyz_to_Yxy(xyz3)
Yxyw = xyz_to_Yxy(xyzw)
# get spectrum locus Y,x,y and wavelengths:
SL = _CMF[cieobs]['bar']
SL = SL[:, SL[1:].sum(axis=0) >
0] # avoid div by zero in xyz-to-Yxy conversion
wlsl = SL[0]
Yxysl = xyz_to_Yxy(SL[1:4].T)[:, None]
# Get maximum wavelength of spectrum locus (before it turns back on itself)
if SL_max_lambda is None:
pmaxlambda = Yxysl[..., 1].argmax() # lambda with largest x value
dwl = np.diff(
Yxysl[:, 0,
1]) # spectrumlocus in that range should have increasing x
dwl[wlsl[:-1] < 600] = 10000
pmaxlambda = np.where(
dwl <= 0)[0][0] # Take first element with zero or <zero slope
else:
pmaxlambda = np.abs(wlsl - SL_max_lambda).argmin()
Yxysl = Yxysl[:(pmaxlambda + 1), :]
wlsl = wlsl[:(pmaxlambda + 1)]
# center on xyzw:
Yxy = Yxy - Yxyw
Yxysl = Yxysl - Yxyw
Yxyw = Yxyw - Yxyw
#split:
Y, x, y = asplit(Yxy)
Yw, xw, yw = asplit(Yxyw)
Ysl, xsl, ysl = asplit(Yxysl)
# calculate hue:
h = math.positive_arctan(x, y, htype='deg')
hsl = math.positive_arctan(xsl, ysl, htype='deg')
hsl_max = hsl[0] # max hue angle at min wavelength
hsl_min = hsl[-1] # min hue angle at max wavelength
if hsl_min < hsl_max: hsl_min += 360
dominantwavelength = np.empty(Y.shape)
purity = np.empty(Y.shape)
for i in range(xyz3.shape[1]):
# find index of complementary wavelengths/hues:
pc = np.where(
(h[:, i] > hsl_max) & (h[:, i] < hsl_min)
) # hue's requiring complementary wavelength (purple line)
h[:, i][pc] = h[:, i][pc] - np.sign(
h[:, i][pc] - 180.0
) * 180.0 # add/subtract 180° to get positive complementary wavelength
# find 2 closest enclosing hues in sl:
#hslb,hib = meshblock(hsl,h[:,i:i+1])
hib, hslb = np.meshgrid(h[:, i:i + 1], hsl)
dh = (hslb - hib)
q1 = np.abs(dh).argmin(axis=0) # index of closest hue
sign_q1 = np.sign(dh[q1])[0]
dh[np.sign(dh) ==
sign_q1] = 1000000 # set all dh on the same side as q1 to a very large value
q2 = np.abs(dh).argmin(
axis=0) # index of second closest (enclosing) hue
# # Test changes to code:
# print('wls',i, wlsl[q1],wlsl[q2])
# import matplotlib.pyplot as plt
# plt.figure()
# plt.plot(wlsl[:-1],np.diff(xsl[:,0]),'k.-')
# plt.figure()
# plt.plot(x[0,i],y[0,i],'k.'); plt.plot(xsl,ysl,'r.-');plt.plot(xsl[q1],ysl[q1],'b.');plt.plot(xsl[q2],ysl[q2],'g.');plt.plot(xsl[-1],ysl[-1],'c+')
dominantwavelength[:, i] = wlsl[q1] + np.multiply(
(h[:, i] - hsl[q1, 0]),
np.divide((wlsl[q2] - wlsl[q1]), (hsl[q2, 0] - hsl[q1, 0]))
) # calculate wl corresponding to h: y = y1 + (x-x1)*(y2-y1)/(x2-x1)
dominantwavelength[:, i][pc] = -dominantwavelength[:, i][
pc] #complementary wavelengths are specified by '-' sign
# calculate excitation purity:
x_dom_wl = xsl[q1, 0] + (xsl[q2, 0] - xsl[q1, 0]) * (h[:, i] - hsl[
q1, 0]) / (hsl[q2, 0] - hsl[q1, 0]) # calculate x of dom. wl
y_dom_wl = ysl[q1, 0] + (ysl[q2, 0] - ysl[q1, 0]) * (h[:, i] - hsl[
q1, 0]) / (hsl[q2, 0] - hsl[q1, 0]) # calculate y of dom. wl
d_wl = (x_dom_wl**2.0 +
y_dom_wl**2.0)**0.5 # distance from white point to sl
d = (x[:, i]**2.0 +
y[:, i]**2.0)**0.5 # distance from white point to test point
purity[:, i] = d / d_wl
# correct for those test points that have a complementary wavelength
# calculate intersection of line through white point and test point and purple line:
xy = np.vstack((x[:, i], y[:, i])).T
xyw = np.hstack((xw, yw))
xypl1 = np.hstack((xsl[0, None], ysl[0, None]))
xypl2 = np.hstack((xsl[-1, None], ysl[-1, None]))
da = (xy - xyw)
db = (xypl2 - xypl1)
dp = (xyw - xypl1)
T = np.array([[0.0, -1.0], [1.0, 0.0]])
dap = np.dot(da, T)
denom = np.sum(dap * db, axis=1, keepdims=True)
num = np.sum(dap * dp, axis=1, keepdims=True)
xy_linecross = (num / denom) * db + xypl1
d_linecross = np.atleast_2d(
(xy_linecross[:, 0]**2.0 + xy_linecross[:, 1]**2.0)**0.5).T #[0]
purity[:, i][pc] = d[pc] / d_linecross[pc][:, 0]
Ydlep = np.dstack((xyz3[:, :, 1], dominantwavelength, purity))
if axes12flipped == True:
Ydlep = Ydlep.transpose((1, 0, 2))
else:
Ydlep = Ydlep.transpose((0, 1, 2))
return Ydlep.reshape(xyz.shape)
def xyz_to_Ydlep_(xyz,
cieobs=_CIEOBS,
xyzw=_COLORTF_DEFAULT_WHITE_POINT,
flip_axes=False,
**kwargs):
"""
Convert XYZ tristimulus values to Y, dominant (complementary) wavelength
and excitation purity.
Args:
:xyz:
| ndarray with tristimulus values
:xyzw:
| None or ndarray with tristimulus values of a single (!) native white point, optional
| None defaults to xyz of CIE D65 using the :cieobs: observer.
:cieobs:
| luxpy._CIEOBS, optional
| CMF set to use when calculating spectrum locus coordinates.
:flip_axes:
| False, optional
| If True: flip axis 0 and axis 1 in Ydelep to increase speed of loop in function.
| (single xyzw with is not flipped!)
Returns:
:Ydlep:
| ndarray with Y, dominant (complementary) wavelength
| and excitation purity
"""
xyz3 = np3d(xyz).copy().astype(np.float)
# flip axis so that shortest dim is on axis0 (save time in looping):
if (xyz3.shape[0] < xyz3.shape[1]) & (flip_axes == True):
axes12flipped = True
xyz3 = xyz3.transpose((1, 0, 2))
else:
axes12flipped = False
# convert xyz to Yxy:
Yxy = xyz_to_Yxy(xyz3)
Yxyw = xyz_to_Yxy(xyzw)
# get spectrum locus Y,x,y and wavelengths:
SL = _CMF[cieobs]['bar']
SL = SL[:, SL[1:].sum(axis=0) >
0] # avoid div by zero in xyz-to-Yxy conversion
wlsl = SL[0]
Yxysl = xyz_to_Yxy(SL[1:4].T)[:, None]
pmaxlambda = Yxysl[..., 1].argmax()
maxlambda = wlsl[pmaxlambda]
maxlambda = 700
print(np.where(wlsl == maxlambda))
pmaxlambda = np.where(wlsl == maxlambda)[0][0]
Yxysl = Yxysl[:(pmaxlambda + 1), :]
wlsl = wlsl[:(pmaxlambda + 1)]
# center on xyzw:
Yxy = Yxy - Yxyw
Yxysl = Yxysl - Yxyw
Yxyw = Yxyw - Yxyw
#split:
Y, x, y = asplit(Yxy)
Yw, xw, yw = asplit(Yxyw)
Ysl, xsl, ysl = asplit(Yxysl)
# calculate hue:
h = math.positive_arctan(x, y, htype='deg')
print(h)
print('rh', h[0, 0] - h[0, 1])
print(wlsl[0], wlsl[-1])
hsl = math.positive_arctan(xsl, ysl, htype='deg')
hsl_max = hsl[0] # max hue angle at min wavelength
hsl_min = hsl[-1] # min hue angle at max wavelength
if hsl_min < hsl_max: hsl_min += 360
dominantwavelength = np.empty(Y.shape)
purity = np.empty(Y.shape)
print('xyz:', xyz)
for i in range(xyz3.shape[1]):
print('\ni:', i, h[:, i], hsl_max, hsl_min)
print(h)
# find index of complementary wavelengths/hues:
pc = np.where(
(h[:, i] > hsl_max) & (h[:, i] < hsl_min)
) # hue's requiring complementary wavelength (purple line)
print('pc', (h[:, i] > hsl_max) & (h[:, i] < hsl_min))
h[:, i][pc] = h[:, i][pc] - np.sign(
h[:, i][pc] - 180.0
) * 180.0 # add/subtract 180° to get positive complementary wavelength
# find 2 closest hues in sl:
#hslb,hib = meshblock(hsl,h[:,i:i+1])
hib, hslb = np.meshgrid(h[:, i:i + 1], hsl)
dh = np.abs(hslb - hib)
q1 = dh.argmin(axis=0) # index of closest hue
dh[q1] = 1000000.0
q2 = dh.argmin(axis=0) # index of second closest hue
print('q1q2', q2, q1)
print('wls:', h[:, i], wlsl[q1], wlsl[q2])
print('hsls:', hsl[q2, 0], hsl[q1, 0])
print('d', (wlsl[q2] - wlsl[q1]), (hsl[q2, 0] - hsl[q1, 0]),
(wlsl[q2] - wlsl[q1]) / (hsl[q2, 0] - hsl[q1, 0]))
print('(h[:,i] - hsl[q1,0])', (h[:, i] - hsl[q1, 0]))
print('div', np.divide((wlsl[q2] - wlsl[q1]),
(hsl[q2, 0] - hsl[q1, 0])))
print(
'mult(...)',
np.multiply((h[:, i] - hsl[q1, 0]),
np.divide((wlsl[q2] - wlsl[q1]),
(hsl[q2, 0] - hsl[q1, 0]))))
dominantwavelength[:, i] = wlsl[q1] + np.multiply(
(h[:, i] - hsl[q1, 0]),
np.divide((wlsl[q2] - wlsl[q1]), (hsl[q2, 0] - hsl[q1, 0]))
) # calculate wl corresponding to h: y = y1 + (x-x1)*(y2-y1)/(x2-x1)
print('dom', dominantwavelength[:, i])
dominantwavelength[(dominantwavelength[:,
i] > max(wlsl[q1], wlsl[q2])),
i] = max(wlsl[q1], wlsl[q2])
dominantwavelength[(dominantwavelength[:,
i] < min(wlsl[q1], wlsl[q2])),
i] = min(wlsl[q1], wlsl[q2])
dominantwavelength[:, i][pc] = -dominantwavelength[:, i][
pc] #complementary wavelengths are specified by '-' sign
# calculate excitation purity:
x_dom_wl = xsl[q1, 0] + (xsl[q2, 0] - xsl[q1, 0]) * (h[:, i] - hsl[
q1, 0]) / (hsl[q2, 0] - hsl[q1, 0]) # calculate x of dom. wl
y_dom_wl = ysl[q1, 0] + (ysl[q2, 0] - ysl[q1, 0]) * (h[:, i] - hsl[
q1, 0]) / (hsl[q2, 0] - hsl[q1, 0]) # calculate y of dom. wl
d_wl = (x_dom_wl**2.0 +
y_dom_wl**2.0)**0.5 # distance from white point to sl
d = (x[:, i]**2.0 +
y[:, i]**2.0)**0.5 # distance from white point to test point
purity[:, i] = d / d_wl
# correct for those test points that have a complementary wavelength
# calculate intersection of line through white point and test point and purple line:
xy = np.vstack((x[:, i], y[:, i])).T
xyw = np.hstack((xw, yw))
xypl1 = np.hstack((xsl[0, None], ysl[0, None]))
xypl2 = np.hstack((xsl[-1, None], ysl[-1, None]))
da = (xy - xyw)
db = (xypl2 - xypl1)
dp = (xyw - xypl1)
T = np.array([[0.0, -1.0], [1.0, 0.0]])
dap = np.dot(da, T)
denom = np.sum(dap * db, axis=1, keepdims=True)
num = np.sum(dap * dp, axis=1, keepdims=True)
xy_linecross = (num / denom) * db + xypl1
d_linecross = np.atleast_2d(
(xy_linecross[:, 0]**2.0 + xy_linecross[:, 1]**2.0)**0.5).T #[0]
purity[:, i][pc] = d[pc] / d_linecross[pc][:, 0]
Ydlep = np.dstack((xyz3[:, :, 1], dominantwavelength, purity))
if axes12flipped == True:
Ydlep = Ydlep.transpose((1, 0, 2))
else:
Ydlep = Ydlep.transpose((0, 1, 2))
return Ydlep.reshape(xyz.shape)
def Ydlep_to_xyz(Ydlep,
cieobs=_CIEOBS,
xyzw=_COLORTF_DEFAULT_WHITE_POINT,
flip_axes=False,
SL_max_lambda=None,
**kwargs):
"""
Convert Y, dominant (complementary) wavelength and excitation purity to XYZ
tristimulus values.
Args:
:Ydlep:
| ndarray with Y, dominant (complementary) wavelength
and excitation purity
:xyzw:
| None or narray with tristimulus values of a single (!) native white point, optional
| None defaults to xyz of CIE D65 using the :cieobs: observer.
:cieobs:
| luxpy._CIEOBS, optional
| CMF set to use when calculating spectrum locus coordinates.
:flip_axes:
| False, optional
| If True: flip axis 0 and axis 1 in Ydelep to increase speed of loop in function.
| (single xyzw with is not flipped!)
:SL_max_lambda:
| None or float, optional
| Maximum wavelength of spectrum locus before it turns back on itelf in the high wavelength range (~700 nm)
Returns:
:xyz:
| ndarray with tristimulus values
"""
Ydlep3 = np3d(Ydlep).copy().astype(np.float)
# flip axis so that longest dim is on first axis (save time in looping):
if (Ydlep3.shape[0] < Ydlep3.shape[1]) & (flip_axes == True):
axes12flipped = True
Ydlep3 = Ydlep3.transpose((1, 0, 2))
else:
axes12flipped = False
# convert xyzw to Yxyw:
Yxyw = xyz_to_Yxy(xyzw)
Yxywo = Yxyw.copy()
# get spectrum locus Y,x,y and wavelengths:
SL = _CMF[cieobs]['bar']
SL = SL[:, SL[1:].sum(axis=0) >
0] # avoid div by zero in xyz-to-Yxy conversion
wlsl = SL[0, None].T
Yxysl = xyz_to_Yxy(SL[1:4].T)[:, None]
# Get maximum wavelength of spectrum locus (before it turns back on itself)
if SL_max_lambda is None:
pmaxlambda = Yxysl[..., 1].argmax() # lambda with largest x value
dwl = np.diff(
Yxysl[:, 0,
1]) # spectrumlocus in that range should have increasing x
dwl[wlsl[:-1, 0] < 600] = 10000
pmaxlambda = np.where(
dwl <= 0)[0][0] # Take first element with zero or <zero slope
else:
pmaxlambda = np.abs(wlsl - SL_max_lambda).argmin()
Yxysl = Yxysl[:(pmaxlambda + 1), :]
wlsl = wlsl[:(pmaxlambda + 1), :1]
# center on xyzw:
Yxysl = Yxysl - Yxyw
Yxyw = Yxyw - Yxyw
#split:
Y, dom, pur = asplit(Ydlep3)
Yw, xw, yw = asplit(Yxyw)
Ywo, xwo, ywo = asplit(Yxywo)
Ysl, xsl, ysl = asplit(Yxysl)
# loop over longest dim:
x = np.empty(Y.shape)
y = np.empty(Y.shape)
for i in range(Ydlep3.shape[1]):
# find closest wl's to dom:
#wlslb,wlib = meshblock(wlsl,np.abs(dom[i,:])) #abs because dom<0--> complemtary wl
wlib, wlslb = np.meshgrid(np.abs(dom[:, i]), wlsl)
dwl = wlslb - wlib
q1 = np.abs(dwl).argmin(axis=0) # index of closest wl
sign_q1 = np.sign(dwl[q1])
dwl[np.sign(dwl) ==
sign_q1] = 1000000 # set all dwl on the same side as q1 to a very large value
q2 = np.abs(dwl).argmin(
axis=0) # index of second closest (enclosing) wl
# calculate x,y of dom:
x_dom_wl = xsl[q1, 0] + (xsl[q2, 0] - xsl[q1, 0]) * (
np.abs(dom[:, i]) - wlsl[q1, 0]) / (wlsl[q2, 0] - wlsl[q1, 0]
) # calculate x of dom. wl
y_dom_wl = ysl[q1, 0] + (ysl[q2, 0] - ysl[q1, 0]) * (
np.abs(dom[:, i]) - wlsl[q1, 0]) / (wlsl[q2, 0] - wlsl[q1, 0]
) # calculate y of dom. wl
# calculate x,y of test:
d_wl = (x_dom_wl**2.0 +
y_dom_wl**2.0)**0.5 # distance from white point to dom
d = pur[:, i] * d_wl
hdom = math.positive_arctan(x_dom_wl, y_dom_wl, htype='deg')
x[:, i] = d * np.cos(hdom * np.pi / 180.0)
y[:, i] = d * np.sin(hdom * np.pi / 180.0)
# complementary:
pc = np.where(dom[:, i] < 0.0)
hdom[pc] = hdom[pc] - np.sign(dom[:, i][pc] -
180.0) * 180.0 # get positive hue angle
# calculate intersection of line through white point and test point and purple line:
xy = np.vstack((x_dom_wl, y_dom_wl)).T
xyw = np.vstack((xw, yw)).T
xypl1 = np.vstack((xsl[0, None], ysl[0, None])).T
xypl2 = np.vstack((xsl[-1, None], ysl[-1, None])).T
da = (xy - xyw)
db = (xypl2 - xypl1)
dp = (xyw - xypl1)
T = np.array([[0.0, -1.0], [1.0, 0.0]])
dap = np.dot(da, T)
denom = np.sum(dap * db, axis=1, keepdims=True)
num = np.sum(dap * dp, axis=1, keepdims=True)
xy_linecross = (num / denom) * db + xypl1
d_linecross = np.atleast_2d(
(xy_linecross[:, 0]**2.0 + xy_linecross[:, 1]**2.0)**0.5).T[:, 0]
x[:, i][pc] = pur[:, i][pc] * d_linecross[pc] * np.cos(
hdom[pc] * np.pi / 180)
y[:, i][pc] = pur[:, i][pc] * d_linecross[pc] * np.sin(
hdom[pc] * np.pi / 180)
Yxy = np.dstack((Ydlep3[:, :, 0], x + xwo, y + ywo))
if axes12flipped == True:
Yxy = Yxy.transpose((1, 0, 2))
else:
Yxy = Yxy.transpose((0, 1, 2))
return Yxy_to_xyz(Yxy).reshape(Ydlep.shape)
def cam15u(data,
fov=10.0,
inputtype='xyz',
direction='forward',
outin='Q,aW,bW',
parameters=None):
"""
Convert between CIE 2006 10° XYZ tristimulus values (or spectral data)
and CAM15u color appearance correlates.
Args:
:data:
| ndarray of CIE 2006 10° XYZ tristimulus values or spectral data
| or color appearance attributes
:fov:
| 10.0, optional
| Field-of-view of stimulus (for size effect on brightness)
:inputtpe:
| 'xyz' or 'spd', optional
| Specifies the type of input:
| tristimulus values or spectral data for the forward mode.
:direction:
| 'forward' or 'inverse', optional
| -'forward': xyz -> cam15u
| -'inverse': cam15u -> xyz
:outin:
| 'Q,aW,bW' or str, optional
| 'Q,aW,bW' (brightness and opponent signals for amount-of-neutral)
| other options: 'Q,aM,bM' (colorfulness) and 'Q,aS,bS' (saturation)
| Str specifying the type of
| input (:direction: == 'inverse') and
| output (:direction: == 'forward')
:parameters:
| None or dict, optional
| Set of model parameters.
| - None: defaults to luxpy.cam._CAM15U_PARAMETERS
| (see references below)
Returns:
:returns:
| ndarray with color appearance correlates (:direction: == 'forward')
| or
| XYZ tristimulus values (:direction: == 'inverse')
References:
1. `M. Withouck, K. A. G. Smet, W. R. Ryckaert, and P. Hanselaer,
“Experimental driven modelling of the color appearance of
unrelated self-luminous stimuli: CAM15u,”
Opt. Express, vol. 23, no. 9, pp. 12045–12064, 2015.
<https://www.osapublishing.org/oe/abstract.cfm?uri=oe-23-9-12045&origin=search>`_
2. `M. Withouck, K. A. G. Smet, and P. Hanselaer, (2015),
“Brightness prediction of different sized unrelated self-luminous stimuli,”
Opt. Express, vol. 23, no. 10, pp. 13455–13466.
<https://www.osapublishing.org/oe/abstract.cfm?uri=oe-23-10-13455&origin=search>`_
"""
if parameters is None:
parameters = _CAM15U_PARAMETERS
outin = outin.split(',')
#unpack model parameters:
Mxyz2rgb, cA, cAlms, cHK, cM, cW, ca, calms, cb, cblms, cfov, cp, k, unique_hue_data = [
parameters[x] for x in sorted(parameters.keys())
]
# precomputations:
invMxyz2rgb = np.linalg.inv(Mxyz2rgb)
MAab = np.array([cAlms, calms, cblms])
invMAab = np.linalg.inv(MAab)
#initialize data and camout:
data = np2d(data)
if len(data.shape) == 2:
data = np.expand_dims(data, axis=0) # avoid looping if not necessary
if (data.shape[0] > data.shape[1]): # loop over shortest dim.
flipaxis0and1 = True
data = np.transpose(data, axes=(1, 0, 2))
else:
flipaxis0and1 = False
dshape = list(data.shape)
dshape[-1] = len(outin) # requested number of correlates
if (inputtype != 'xyz') & (direction == 'forward'):
dshape[-2] = dshape[
-2] - 1 # wavelength row doesn't count & only with forward can the input data be spectral
camout = np.zeros(dshape)
camout.fill(np.nan)
for i in range(data.shape[0]):
if (inputtype != 'xyz') & (direction == 'forward'):
xyz = spd_to_xyz(data[i], cieobs='2006_10', relative=False)
lms = np.dot(_CMF['2006_10']['M'], xyz.T).T # convert to l,m,s
rgb = (lms /
_CMF['2006_10']['K']) * k # convert to rho, gamma, beta
elif (inputtype == 'xyz') & (direction == 'forward'):
rgb = np.dot(Mxyz2rgb, data[i].T).T
if direction == 'forward':
# apply cube-root compression:
rgbc = rgb**(cp)
# calculate achromatic and color difference signals, A, a, b:
Aab = np.dot(MAab, rgbc.T).T
A, a, b = asplit(Aab)
A = cA * A
a = ca * a
b = cb * b
# calculate colorfullness like signal M:
M = cM * ((a**2.0 + b**2.0)**0.5)
# calculate brightness Q:
Q = A + cHK[0] * M**cHK[
1] # last term is contribution of Helmholtz-Kohlrausch effect on brightness
# calculate saturation, s:
s = M / Q
# calculate amount of white, W:
W = 100.0 / (1.0 + cW[0] * (s**cW[1]))
# adjust Q for size (fov) of stimulus (matter of debate whether to do this before or after calculation of s or W, there was no data on s, M or W for different sized stimuli: after)
Q = Q * (fov / 10.0)**cfov
# calculate hue, h and Hue quadrature, H:
h = hue_angle(a, b, htype='deg')
if 'H' in outin:
H = hue_quadrature(h, unique_hue_data=unique_hue_data)
else:
H = None
# calculate cart. co.:
if 'aM' in outin:
aM = M * np.cos(h * np.pi / 180.0)
bM = M * np.sin(h * np.pi / 180.0)
if 'aS' in outin:
aS = s * np.cos(h * np.pi / 180.0)
bS = s * np.sin(h * np.pi / 180.0)
if 'aW' in outin:
aW = W * np.cos(h * np.pi / 180.0)
bW = W * np.sin(h * np.pi / 180.0)
if (outin != ['Q', 'aW', 'bW']):
camout[i] = eval('ajoin((' + ','.join(outin) + '))')
else:
camout[i] = ajoin((Q, aW, bW))
elif direction == 'inverse':
# get Q, M and a, b depending on input type:
if 'aW' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
W = (a**2.0 + b**2.0)**0.5
s = (((100 / W) - 1.0) / cW[0])**(1.0 / cW[1])
M = s * Q
if 'aM' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
M = (a**2.0 + b**2.0)**0.5
if 'aS' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
s = (a**2.0 + b**2.0)**0.5
M = s * Q
if 'h' in outin:
Q, WsM, h = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
if 'W' in outin:
s = (((100.0 / WsM) - 1.0) / cW[0])**(1.0 / cW[1])
M = s * Q
elif 's' in outin:
M = WsM * Q
elif 'M' in outin:
M = WsM
# calculate achromatic signal, A from Q and M:
A = Q - cHK[0] * M**cHK[1]
A = A / cA
# calculate hue angle:
h = hue_angle(a, b, htype='rad')
# calculate a,b from M and h:
a = (M / cM) * np.cos(h)
b = (M / cM) * np.sin(h)
a = a / ca
b = b / cb
# create Aab:
Aab = ajoin((A, a, b))
# calculate rgbc:
rgbc = np.dot(invMAab, Aab.T).T
# decompress rgbc to rgb:
rgb = rgbc**(1 / cp)
# convert rgb to xyz:
xyz = np.dot(invMxyz2rgb, rgb.T).T
camout[i] = xyz
if flipaxis0and1 == True: # loop over shortest dim.
camout = np.transpose(camout, axes=(1, 0, 2))
if camout.shape[0] == 1:
camout = np.squeeze(camout, axis=0)
return camout
def cam_sww16(data, dataw = None, Yb = 20.0, Lw = 400.0, Ccwb = None, relative = True, \
parameters = None, inputtype = 'xyz', direction = 'forward', \
cieobs = '2006_10'):
"""
A simple principled color appearance model based on a mapping
of the Munsell color system.
| This function implements the JOSA A (parameters = 'JOSA') published model.
Args:
:data:
| ndarray with input tristimulus values
| or spectral data
| or input color appearance correlates
| Can be of shape: (N [, xM], x 3), whereby:
| N refers to samples and M refers to light sources.
| Note that for spectral input shape is (N x (M+1) x wl)
:dataw:
| None or ndarray, optional
| Input tristimulus values or spectral data of white point.
| None defaults to the use of CIE illuminant C.
:Yb:
| 20.0, optional
| Luminance factor of background (perfect white diffuser, Yw = 100)
:Lw:
| 400.0, optional
| Luminance (cd/m²) of white point.
:Ccwb:
| None, optional
| Degree of cognitive adaptation (white point balancing)
| If None: use [..,..] from parameters dict.
:relative:
| True or False, optional
| True: xyz tristimulus values are relative (Yw = 100)
:parameters:
| None or str or dict, optional
| Dict with model parameters.
| - None: defaults to luxpy.cam._CAM_SWW_2016_PARAMETERS['JOSA']
| - str: 'best-fit-JOSA' or 'best-fit-all-Munsell'
| - dict: user defined model parameters
| (dict should have same structure)
:inputtype:
| 'xyz' or 'spd', optional
| Specifies the type of input:
| tristimulus values or spectral data for the forward mode.
:direction:
| 'forward' or 'inverse', optional
| -'forward': xyz -> cam_sww_2016
| -'inverse': cam_sww_2016 -> xyz
:cieobs:
| '2006_10', optional
| CMF set to use to perform calculations where spectral data
is involved (inputtype == 'spd'; dataw = None)
| Other options: see luxpy._CMF['types']
Returns:
:returns:
| ndarray with color appearance correlates (:direction: == 'forward')
| or
| XYZ tristimulus values (:direction: == 'inverse')
Notes:
| This function implements the JOSA A (parameters = 'JOSA')
published model.
| With:
| 1. A correction for the parameter
| in Eq.4 of Fig. 11: 0.952 --> -0.952
|
| 2. The delta_ac and delta_bc white-balance shifts in Eq. 5e & 5f
| should be: -0.028 & 0.821
|
| (cfr. Ccwb = 0.66 in:
| ab_test_out = ab_test_int - Ccwb*ab_gray_adaptation_field_int))
References:
1. `Smet, K. A. G., Webster, M. A., & Whitehead, L. A. (2016).
A simple principled approach for modeling and understanding uniform color metrics.
Journal of the Optical Society of America A, 33(3), A319–A331.
<https://doi.org/10.1364/JOSAA.33.00A319>`_
"""
# get model parameters
args = locals().copy()
if parameters is None:
parameters = _CAM_SWW16_PARAMETERS['JOSA']
if isinstance(parameters, str):
parameters = _CAM_SWW16_PARAMETERS[parameters]
parameters = put_args_in_db(
parameters,
args) #overwrite parameters with other (not-None) args input
#unpack model parameters:
Cc, Ccwb, Cf, Mxyz2lms, cLMS, cab_int, cab_out, calpha, cbeta, cga1, cga2, cgb1, cgb2, cl_int, clambda, lms0 = [
parameters[x] for x in sorted(parameters.keys())
]
# setup default adaptation field:
if (dataw is None):
dataw = _CIE_ILLUMINANTS['C'].copy() # get illuminant C
xyzw = spd_to_xyz(dataw, cieobs=cieobs,
relative=False) # get abs. tristimulus values
if relative == False: #input is expected to be absolute
dataw[1:] = Lw * dataw[
1:] / xyzw[:, 1:2] #dataw = Lw*dataw # make absolute
else:
dataw = dataw # make relative (Y=100)
if inputtype == 'xyz':
dataw = spd_to_xyz(dataw, cieobs=cieobs, relative=relative)
# precomputations:
Mxyz2lms = np.dot(
np.diag(cLMS),
math.normalize_3x3_matrix(Mxyz2lms, np.array([[1, 1, 1]]))
) # normalize matrix for xyz-> lms conversion to ill. E weighted with cLMS
invMxyz2lms = np.linalg.inv(Mxyz2lms)
MAab = np.array([clambda, calpha, cbeta])
invMAab = np.linalg.inv(MAab)
#initialize data and camout:
data = np2d(data).copy(
) # stimulus data (can be upto NxMx3 for xyz, or [N x (M+1) x wl] for spd))
dataw = np2d(dataw).copy(
) # white point (can be upto Nx3 for xyz, or [(N+1) x wl] for spd)
# make axis 1 of dataw have 'same' dimensions as data:
if (data.ndim == 2):
data = np.expand_dims(data, axis=1) # add light source axis 1
if inputtype == 'xyz':
if dataw.shape[
0] == 1: #make dataw have same lights source dimension size as data
dataw = np.repeat(dataw, data.shape[1], axis=0)
else:
if dataw.shape[0] == 2:
dataw = np.vstack(
(dataw[0], np.repeat(dataw[1:], data.shape[1], axis=0)))
# Flip light source dim to axis 0:
data = np.transpose(data, axes=(1, 0, 2))
# Initialize output array:
dshape = list(data.shape)
dshape[-1] = 3 # requested number of correlates: l_int, a_int, b_int
if (inputtype != 'xyz') & (direction == 'forward'):
dshape[-2] = dshape[
-2] - 1 # wavelength row doesn't count & only with forward can the input data be spectral
camout = np.zeros(dshape)
camout.fill(np.nan)
# apply forward/inverse model for each row in data:
for i in range(data.shape[0]):
# stage 1: calculate photon rates of stimulus and adapting field, lmst & lmsf:
if (inputtype != 'xyz'):
if relative == True:
xyzw_abs = spd_to_xyz(np.vstack((dataw[0], dataw[i + 1])),
cieobs=cieobs,
relative=False)
dataw[i +
1] = Lw * dataw[i + 1] / xyzw_abs[0, 1] # make absolute
xyzw = spd_to_xyz(np.vstack((dataw[0], dataw[i + 1])),
cieobs=cieobs,
relative=False)
lmsw = 683.0 * np.dot(Mxyz2lms, xyzw.T).T / _CMF[cieobs]['K']
lmsf = (Yb / 100.0
) * lmsw # calculate adaptation field and convert to l,m,s
if (direction == 'forward'):
if relative == True:
data[i, 1:, :] = Lw * data[i, 1:, :] / xyzw_abs[
0, 1] # make absolute
xyzt = spd_to_xyz(data[i], cieobs=cieobs,
relative=False) / _CMF[cieobs]['K']
lmst = 683.0 * np.dot(Mxyz2lms, xyzt.T).T # convert to l,m,s
else:
lmst = lmsf # put lmsf in lmst for inverse-mode
elif (inputtype == 'xyz'):
if relative == True:
dataw[i] = Lw * dataw[i] / 100.0 # make absolute
lmsw = 683.0 * np.dot(
Mxyz2lms, dataw[i].T).T / _CMF[cieobs]['K'] # convert to lms
lmsf = (Yb / 100.0) * lmsw
if (direction == 'forward'):
if relative == True:
data[i] = Lw * data[i] / 100.0 # make absolute
lmst = 683.0 * np.dot(
Mxyz2lms,
data[i].T).T / _CMF[cieobs]['K'] # convert to lms
else:
lmst = lmsf # put lmsf in lmst for inverse-mode
# stage 2: calculate cone outputs of stimulus lmstp
lmstp = math.erf(Cc * (np.log(lmst / lms0) + Cf * np.log(lmsf / lms0)))
lmsfp = math.erf(Cc * (np.log(lmsf / lms0) + Cf * np.log(lmsf / lms0)))
lmstp = np.vstack(
(lmsfp, lmstp)
) # add adaptation field lms temporarily to lmsp for quick calculation
# stage 3: calculate optic nerve signals, lam*, alphp, betp:
lstar, alph, bet = asplit(np.dot(MAab, lmstp.T).T)
alphp = cga1[0] * alph
alphp[alph < 0] = cga1[1] * alph[alph < 0]
betp = cgb1[0] * bet
betp[bet < 0] = cgb1[1] * bet[bet < 0]
# stage 4: calculate recoded nerve signals, alphapp, betapp:
alphpp = cga2[0] * (alphp + betp)
betpp = cgb2[0] * (alphp - betp)
# stage 5: calculate conscious color perception:
lstar_int = cl_int[0] * (lstar + cl_int[1])
alph_int = cab_int[0] * (np.cos(cab_int[1] * np.pi / 180.0) * alphpp -
np.sin(cab_int[1] * np.pi / 180.0) * betpp)
bet_int = cab_int[0] * (np.sin(cab_int[1] * np.pi / 180.0) * alphpp +
np.cos(cab_int[1] * np.pi / 180.0) * betpp)
lstar_out = lstar_int
if direction == 'forward':
if Ccwb is None:
alph_out = alph_int - cab_out[0]
bet_out = bet_int - cab_out[1]
else:
Ccwb = Ccwb * np.ones((2))
Ccwb[Ccwb < 0.0] = 0.0
Ccwb[Ccwb > 1.0] = 1.0
alph_out = alph_int - Ccwb[0] * alph_int[
0] # white balance shift using adaptation gray background (Yb=20%), with Ccw: degree of adaptation
bet_out = bet_int - Ccwb[1] * bet_int[0]
camout[i] = np.vstack(
(lstar_out[1:], alph_out[1:], bet_out[1:])
).T # stack together and remove adaptation field from vertical stack
elif direction == 'inverse':
labf_int = np.hstack((lstar_int[0], alph_int[0], bet_int[0]))
# get lstar_out, alph_out & bet_out for data:
lstar_out, alph_out, bet_out = asplit(data[i])
# stage 5 inverse:
# undo cortical white-balance:
if Ccwb is None:
alph_int = alph_out + cab_out[0]
bet_int = bet_out + cab_out[1]
else:
Ccwb = Ccwb * np.ones((2))
Ccwb[Ccwb < 0.0] = 0.0
Ccwb[Ccwb > 1.0] = 1.0
alph_int = alph_out + Ccwb[0] * alph_int[
0] # inverse white balance shift using adaptation gray background (Yb=20%), with Ccw: degree of adaptation
bet_int = bet_out + Ccwb[1] * bet_int[0]
lstar_int = lstar_out
alphpp = (1.0 / cab_int[0]) * (
np.cos(-cab_int[1] * np.pi / 180.0) * alph_int -
np.sin(-cab_int[1] * np.pi / 180.0) * bet_int)
betpp = (1.0 / cab_int[0]) * (
np.sin(-cab_int[1] * np.pi / 180.0) * alph_int +
np.cos(-cab_int[1] * np.pi / 180.0) * bet_int)
lstar_int = lstar_out
lstar = (lstar_int / cl_int[0]) - cl_int[1]
# stage 4 inverse:
alphp = 0.5 * (alphpp / cga2[0] + betpp / cgb2[0]
) # <-- alphpp = (Cga2.*(alphp+betp));
betp = 0.5 * (alphpp / cga2[0] - betpp / cgb2[0]
) # <-- betpp = (Cgb2.*(alphp-betp));
# stage 3 invers:
alph = alphp / cga1[0]
bet = betp / cgb1[0]
sa = np.sign(cga1[1])
sb = np.sign(cgb1[1])
alph[(sa * alphp) < 0.0] = alphp[(sa * alphp) < 0] / cga1[1]
bet[(sb * betp) < 0.0] = betp[(sb * betp) < 0] / cgb1[1]
lab = ajoin((lstar, alph, bet))
# stage 2 inverse:
lmstp = np.dot(invMAab, lab.T).T
lmstp[lmstp < -1.0] = -1.0
lmstp[lmstp > 1.0] = 1.0
lmstp = math.erfinv(lmstp) / Cc - Cf * np.log(lmsf / lms0)
lmst = np.exp(lmstp) * lms0
# stage 1 inverse:
xyzt = np.dot(invMxyz2lms, lmst.T).T
if relative == True:
xyzt = (100.0 / Lw) * xyzt
camout[i] = xyzt
# if flipaxis0and1 == True: # loop over shortest dim.
# camout = np.transpose(camout, axes = (1,0,2))
# Flip light source dim back to axis 1:
camout = np.transpose(camout, axes=(1, 0, 2))
if camout.shape[0] == 1:
camout = np.squeeze(camout, axis=0)
return camout
def cam_sww16(data,
dataw=None,
Yb=20.0,
Lw=400.0,
Ccwb=None,
relative=True,
inputtype='xyz',
direction='forward',
parameters=None,
cieobs='2006_10',
match_to_conversionmatrix_to_cieobs=True):
"""
A simple principled color appearance model based on a mapping of
the Munsell color system.
| This function implements the JOSA A (parameters = 'JOSA') published model.
Args:
:data:
| ndarray with input tristimulus values
| or spectral data
| or input color appearance correlates
| Can be of shape: (N [, xM], x 3), whereby:
| N refers to samples and M refers to light sources.
| Note that for spectral input shape is (N x (M+1) x wl)
:dataw:
| None or ndarray, optional
| Input tristimulus values or spectral data of white point.
| None defaults to the use of CIE illuminant C.
:Yb:
| 20.0, optional
| Luminance factor of background (perfect white diffuser, Yw = 100)
:Lw:
| 400.0, optional
| Luminance (cd/m²) of white point.
:Ccwb:
| None, optional
| Degree of cognitive adaptation (white point balancing)
| If None: use [..,..] from parameters dict.
:relative:
| True or False, optional
| True: xyz tristimulus values are relative (Yw = 100)
:parameters:
| None or str or dict, optional
| Dict with model parameters.
| - None: defaults to luxpy.cam._CAM_SWW_2016_PARAMETERS['JOSA']
| - str: 'best-fit-JOSA' or 'best-fit-all-Munsell'
| - dict: user defined model parameters
| (dict should have same structure)
:inputtype:
| 'xyz' or 'spd', optional
| Specifies the type of input:
| tristimulus values or spectral data for the forward mode.
:direction:
| 'forward' or 'inverse', optional
| -'forward': xyz -> cam_sww_2016
| -'inverse': cam_sww_2016 -> xyz
:cieobs:
| '2006_10', optional
| CMF set to use to perform calculations where spectral data
| is involved (inputtype == 'spd'; dataw = None)
| Other options: see luxpy._CMF['types']
:match_to_conversionmatrix_to_cieobs:
| When channging to a different CIE observer, change the xyz-to_lms
| matrix to the one corresponding to that observer. If False: use
| the one set in parameters or _CAM_SWW16_PARAMETERS
Returns:
:returns:
| ndarray with color appearance correlates (:direction: == 'forward')
| or
| XYZ tristimulus values (:direction: == 'inverse')
Notes:
| This function implements the JOSA A (parameters = 'JOSA')
| published model.
| With:
| 1. A correction for the parameter
| in Eq.4 of Fig. 11: 0.952 --> -0.952
|
| 2. The delta_ac and delta_bc white-balance shifts in Eq. 5e & 5f
| should be: -0.028 & 0.821
|
| (cfr. Ccwb = 0.66 in:
| ab_test_out = ab_test_int - Ccwb*ab_gray_adaptation_field_int))
References:
1. `Smet, K. A. G., Webster, M. A., & Whitehead, L. A. (2016).
A simple principled approach for modeling and understanding uniform color metrics.
Journal of the Optical Society of America A, 33(3), A319–A331.
<https://doi.org/10.1364/JOSAA.33.00A319>`_
"""
#--------------------------------------------------------------------------
# Get model parameters:
#--------------------------------------------------------------------------
args = locals().copy()
parameters = _update_parameter_dict(
args,
parameters=parameters,
match_to_conversionmatrix_to_cieobs=match_to_conversionmatrix_to_cieobs
)
#unpack model parameters:
Cc, Ccwb, Cf, Mxyz2lms, cLMS, cab_int, cab_out, calpha, cbeta, cga1, cga2, cgb1, cgb2, cl_int, clambda, lms0 = [
parameters[x] for x in sorted(parameters.keys())
]
#--------------------------------------------------------------------------
# Setup default adaptation field:
#--------------------------------------------------------------------------
dataw = _setup_default_adaptation_field(dataw=dataw,
Lw=Lw,
inputtype=inputtype,
relative=relative,
cieobs=cieobs)
#--------------------------------------------------------------------------
# Redimension input data to ensure most appropriate sizes
# for easy and efficient looping and initialize output array:
#--------------------------------------------------------------------------
data, dataw, camout, originalshape = _massage_input_and_init_output(
data, dataw, inputtype=inputtype, direction=direction)
#--------------------------------------------------------------------------
# Do precomputations needed for both the forward and inverse model,
# and which do not depend on sample or light source data:
#--------------------------------------------------------------------------
Mxyz2lms = np.dot(
np.diag(cLMS), Mxyz2lms
) # weight the xyz-to-lms conversion matrix with cLMS (cfr. stage 1 calculations)
invMxyz2lms = np.linalg.inv(
Mxyz2lms) # Calculate the inverse lms-to-xyz conversion matrix
MAab = np.array(
[clambda, calpha, cbeta]
) # Create matrix with scale factors for L, M, S for quick matrix multiplications
invMAab = np.linalg.inv(
MAab) # Pre-calculate its inverse to avoid repeat in loop.
#--------------------------------------------------------------------------
# Apply forward/inverse model by looping over each row (=light source dim.)
# in data:
#--------------------------------------------------------------------------
N = data.shape[0]
for i in range(N):
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
# START FORWARD MODE and common part of inverse mode
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
#-----------------------------------------------------------------------------
# Get absolute tristimulus values for stimulus field and white point for row i:
#-----------------------------------------------------------------------------
xyzt, xyzw, xyzw_abs = _get_absolute_xyz_xyzw(data,
dataw,
i=i,
Lw=Lw,
direction=direction,
cieobs=cieobs,
inputtype=inputtype,
relative=relative)
#-----------------------------------------------------------------------------
# stage 1: calculate photon rates of stimulus and white white, and
# adapting field: i.e. lmst, lmsw and lmsf
#-----------------------------------------------------------------------------
# Convert to white point l,m,s:
lmsw = 683.0 * np.dot(Mxyz2lms, xyzw.T).T / _CMF[cieobs]['K']
# Calculate adaptation field and convert to l,m,s:
lmsf = (Yb / 100.0) * lmsw
# Calculate lms of stimulus
# or put adaptation lmsf in test field lmst for later use in inverse-mode (no xyz in 'inverse' mode!!!):
lmst = (683.0 * np.dot(Mxyz2lms, xyzt.T).T /
_CMF[cieobs]['K']) if (direction == 'forward') else lmsf
#-----------------------------------------------------------------------------
# stage 2: calculate cone outputs of stimulus lmstp
#-----------------------------------------------------------------------------
lmstp = math.erf(Cc *
(np.log(lmst / lms0) +
Cf * np.log(lmsf / lms0))) # stimulus test field
lmsfp = math.erf(Cc * (np.log(lmsf / lms0) +
Cf * np.log(lmsf / lms0))) # adaptation field
# add adaptation field lms temporarily to lmstp for quick calculation
lmstp = np.vstack((lmsfp, lmstp))
#-----------------------------------------------------------------------------
# stage 3: calculate optic nerve signals, lam*, alphp, betp:
#-----------------------------------------------------------------------------
lstar, alph, bet = asplit(np.dot(MAab, lmstp.T).T)
alphp = cga1[0] * alph
alphp[alph < 0] = cga1[1] * alph[alph < 0]
betp = cgb1[0] * bet
betp[bet < 0] = cgb1[1] * bet[bet < 0]
#-----------------------------------------------------------------------------
# stage 4: calculate recoded nerve signals, alphapp, betapp:
#-----------------------------------------------------------------------------
alphpp = cga2[0] * (alphp + betp)
betpp = cgb2[0] * (alphp - betp)
#-----------------------------------------------------------------------------
# stage 5: calculate conscious color perception:
#-----------------------------------------------------------------------------
lstar_int = cl_int[0] * (lstar + cl_int[1])
alph_int = cab_int[0] * (np.cos(cab_int[1] * np.pi / 180.0) * alphpp -
np.sin(cab_int[1] * np.pi / 180.0) * betpp)
bet_int = cab_int[0] * (np.sin(cab_int[1] * np.pi / 180.0) * alphpp +
np.cos(cab_int[1] * np.pi / 180.0) * betpp)
lstar_out = lstar_int
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
# stage 5 continued but SPLIT IN FORWARD AND INVERSE MODES:
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
#--------------------------------------
# FORWARD MODE TO PERCEPTUAL SIGNALS:
#--------------------------------------
if direction == 'forward':
if Ccwb is None:
alph_out = alph_int - cab_out[0]
bet_out = bet_int - cab_out[1]
else:
Ccwb = Ccwb * np.ones((2))
Ccwb[Ccwb < 0.0] = 0.0
Ccwb[Ccwb > 1.0] = 1.0
# white balance shift using adaptation gray background (Yb=20%), with Ccw: degree of adaptation:
alph_out = alph_int - Ccwb[0] * alph_int[0]
bet_out = bet_int - Ccwb[1] * bet_int[0]
# stack together and remove adaptation field from vertical stack
# camout is an ndarray with perceptual signals:
camout[i] = np.vstack((lstar_out[1:], alph_out[1:], bet_out[1:])).T
#--------------------------------------
# INVERSE MODE FROM PERCEPTUAL SIGNALS:
#--------------------------------------
elif direction == 'inverse':
# stack cognitive pre-adapted adaptation field signals (first on stack) together:
#labf_int = np.hstack((lstar_int[0],alph_int[0],bet_int[0]))
# get lstar_out, alph_out & bet_out for data
#(contains model perceptual signals in inverse mode!!!):
lstar_out, alph_out, bet_out = asplit(data[i])
#------------------------------------------------------------------------
# Inverse stage 5: undo cortical white-balance:
#------------------------------------------------------------------------
if Ccwb is None:
alph_int = alph_out + cab_out[0]
bet_int = bet_out + cab_out[1]
else:
Ccwb = Ccwb * np.ones((2))
Ccwb[Ccwb < 0.0] = 0.0
Ccwb[Ccwb > 1.0] = 1.0
# inverse white balance shift using adaptation gray background (Yb=20%), with Ccw: degree of adaptation
alph_int = alph_out + Ccwb[0] * alph_int[0]
bet_int = bet_out + Ccwb[1] * bet_int[0]
alphpp = (1.0 / cab_int[0]) * (
np.cos(-cab_int[1] * np.pi / 180.0) * alph_int -
np.sin(-cab_int[1] * np.pi / 180.0) * bet_int)
betpp = (1.0 / cab_int[0]) * (
np.sin(-cab_int[1] * np.pi / 180.0) * alph_int +
np.cos(-cab_int[1] * np.pi / 180.0) * bet_int)
lstar_int = lstar_out
lstar = (lstar_int / cl_int[0]) - cl_int[1]
#---------------------------------------------------------------------------
# Inverse stage 4: pre-adapted perceptual signals to recoded nerve signals:
#---------------------------------------------------------------------------
alphp = 0.5 * (alphpp / cga2[0] + betpp / cgb2[0]
) # <-- alphpp = (Cga2.*(alphp+betp));
betp = 0.5 * (alphpp / cga2[0] - betpp / cgb2[0]
) # <-- betpp = (Cgb2.*(alphp-betp));
#---------------------------------------------------------------------------
# Inverse stage 3: recoded nerve signals to optic nerve signals:
#---------------------------------------------------------------------------
alph = alphp / cga1[0]
bet = betp / cgb1[0]
sa = np.sign(cga1[1])
sb = np.sign(cgb1[1])
alph[(sa * alphp) < 0.0] = alphp[(sa * alphp) < 0] / cga1[1]
bet[(sb * betp) < 0.0] = betp[(sb * betp) < 0] / cgb1[1]
lab = ajoin((lstar, alph, bet))
#---------------------------------------------------------------------------
# Inverse stage 2: optic nerve signals to cone outputs:
#---------------------------------------------------------------------------
lmstp = np.dot(invMAab, lab.T).T
lmstp[lmstp < -1.0] = -1.0
lmstp[lmstp > 1.0] = 1.0
#---------------------------------------------------------------------------
# Inverse stage 1: cone outputs to photon rates:
#---------------------------------------------------------------------------
lmstp = math.erfinv(lmstp) / Cc - Cf * np.log(lmsf / lms0)
lmst = np.exp(lmstp) * lms0
#---------------------------------------------------------------------------
# Photon rates to absolute or relative tristimulus values:
#---------------------------------------------------------------------------
xyzt = np.dot(invMxyz2lms, lmst.T).T * (_CMF[cieobs]['K'] / 683.0)
if relative == True:
xyzt = (100 / Lw) * xyzt
# store in same named variable as forward mode:
camout[i] = xyzt
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
# END inverse mode
#++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
return _massage_output_data_to_original_shape(camout, originalshape)
def cam18sl(data,
datab=None,
Lb=[100],
fov=10.0,
inputtype='xyz',
direction='forward',
outin='Q,aS,bS',
parameters=None):
"""
Convert between CIE 2006 10° XYZ tristimulus values (or spectral data)
and CAM18sl color appearance correlates.
Args:
:data:
| ndarray of CIE 2006 10° absolute XYZ tristimulus values or spectral data
| or color appearance attributes of stimulus
:datab:
| ndarray of CIE 2006 10° absolute XYZ tristimulus values or spectral data
| of stimulus background
:Lb:
| [100], optional
| Luminance (cd/m²) value(s) of background(s) calculated using the CIE 2006 10° CMFs
| (only used in case datab == None and the background is assumed to be an Equal-Energy-White)
:fov:
| 10.0, optional
| Field-of-view of stimulus (for size effect on brightness)
:inputtpe:
| 'xyz' or 'spd', optional
| Specifies the type of input:
| tristimulus values or spectral data for the forward mode.
:direction:
| 'forward' or 'inverse', optional
| -'forward': xyz -> cam18sl
| -'inverse': cam18sl -> xyz
:outin:
| 'Q,aS,bS' or str, optional
| 'Q,aS,bS' (brightness and opponent signals for saturation)
| other options: 'Q,aM,bM' (colorfulness)
| (Note that 'Q,aW,bW' would lead to a Cartesian
| a,b-coordinate system centered at (1,0))
| Str specifying the type of
| input (:direction: == 'inverse') and
| output (:direction: == 'forward')
:parameters:
| None or dict, optional
| Set of model parameters.
| - None: defaults to luxpy.cam._CAM18SL_PARAMETERS
| (see references below)
Returns:
:returns:
| ndarray with color appearance correlates (:direction: == 'forward')
| or
| XYZ tristimulus values (:direction: == 'inverse')
Notes:
| * Instead of using the CIE 1964 10° CMFs in some places of the model,
| the CIE 2006 10° CMFs are used througout, making it more self_consistent.
| This has an effect on the k scaling factors (now different those in CAM15u)
| and the illuminant E normalization for use in the chromatic adaptation transform.
| (see future erratum to Hermans et al., 2018)
| * The paper also used an equation for the amount of white W, which is
| based on a Q value not expressed in 'bright' ('cA' = 0.937 instead of 123).
| This has been corrected for in the luxpy version of the model, i.e.
| _CAM18SL_PARAMETERS['cW'][0] has been changed from 2.29 to 1/11672.
| (see future erratum to Hermans et al., 2018)
| * Default output was 'Q,aW,bW' prior to March 2020, but since this
| is an a,b Cartesian system centered on (1,0), the default output
| has been changed to 'Q,aS,bS'.
References:
1. `Hermans, S., Smet, K. A. G., & Hanselaer, P. (2018).
"Color appearance model for self-luminous stimuli."
Journal of the Optical Society of America A, 35(12), 2000–2009.
<https://doi.org/10.1364/JOSAA.35.002000>`_
"""
if parameters is None:
parameters = _CAM18SL_PARAMETERS
outin = outin.split(',')
#unpack model parameters:
cA, cAlms, cHK, cM, cW, ca, calms, cb, cblms, cfov, cieobs, k, naka, unique_hue_data = [
parameters[x] for x in sorted(parameters.keys())
]
# precomputations:
Mlms2xyz = np.linalg.inv(_CMF[cieobs]['M'])
MAab = np.array([cAlms, calms, cblms])
invMAab = np.linalg.inv(MAab)
#-------------------------------------------------
# setup EEW reference field and default background field (Lr should be equal to Lb):
# Get Lb values:
if datab is not None:
if inputtype != 'xyz':
Lb = spd_to_xyz(datab, cieobs=cieobs, relative=False)[..., 1:2]
else:
Lb = datab[..., 1:2]
else:
if isinstance(Lb, list):
Lb = np2dT(Lb)
# Setup EEW ref of same luminance as datab:
if inputtype == 'xyz':
wlr = getwlr(_CAM18SL_WL3)
else:
if datab is None:
wlr = data[0] # use wlr of stimulus data
else:
wlr = datab[0] # use wlr of background data
datar = np.vstack((wlr, np.ones(
(Lb.shape[0], wlr.shape[0])))) # create eew
xyzr = spd_to_xyz(datar, cieobs=cieobs,
relative=False) # get abs. tristimulus values
datar[1:] = datar[1:] / xyzr[..., 1:2] * Lb
# Create datab if None:
if (datab is None):
if inputtype != 'xyz':
datab = datar.copy()
else:
datab = spd_to_xyz(datar, cieobs=cieobs, relative=False)
# prepare data and datab for loop over backgrounds:
# make axis 1 of datab have 'same' dimensions as data:
if (data.ndim == 2):
data = np.expand_dims(data, axis=1) # add light source axis 1
if inputtype == 'xyz':
datar = spd_to_xyz(datar, cieobs=cieobs,
relative=False) # convert to xyz!!
if datab.shape[
0] == 1: #make datab and datar have same lights source dimension (used to store different backgrounds) size as data
datab = np.repeat(datab, data.shape[1], axis=0)
datar = np.repeat(datar, data.shape[1], axis=0)
else:
if datab.shape[0] == 2:
datab = np.vstack(
(datab[0], np.repeat(datab[1:], data.shape[1], axis=0)))
if datar.shape[0] == 2:
datar = np.vstack(
(datar[0], np.repeat(datar[1:], data.shape[1], axis=0)))
# Flip light source/ background dim to axis 0:
data = np.transpose(data, axes=(1, 0, 2))
#-------------------------------------------------
#initialize camout:
dshape = list(data.shape)
dshape[-1] = len(outin) # requested number of correlates
if (inputtype != 'xyz') & (direction == 'forward'):
dshape[-2] = dshape[
-2] - 1 # wavelength row doesn't count & only with forward can the input data be spectral
camout = np.zeros(dshape)
camout.fill(np.nan)
for i in range(data.shape[0]):
# get rho, gamma, beta of background and reference white:
if (inputtype != 'xyz'):
xyzb = spd_to_xyz(np.vstack((datab[0], datab[i + 1:i + 2, :])),
cieobs=cieobs,
relative=False)
xyzr = spd_to_xyz(np.vstack((datar[0], datar[i + 1:i + 2, :])),
cieobs=cieobs,
relative=False)
else:
xyzb = datab[i:i + 1, :]
xyzr = datar[i:i + 1, :]
lmsb = np.dot(_CMF[cieobs]['M'], xyzb.T).T # convert to l,m,s
rgbb = (lmsb / _CMF[cieobs]['K']) * k # convert to rho, gamma, beta
#lmsr = np.dot(_CMF[cieobs]['M'],xyzr.T).T # convert to l,m,s
#rgbr = (lmsr / _CMF[cieobs]['K']) * k # convert to rho, gamma, beta
#rgbr = rgbr/rgbr[...,1:2]*Lb[i] # calculated EEW cone excitations at same luminance values as background
rgbr = np.ones(xyzr.shape) * Lb[
i] # explicitely equal EEW cone excitations at same luminance values as background
if direction == 'forward':
# get rho, gamma, beta of stimulus:
if (inputtype != 'xyz'):
xyz = spd_to_xyz(data[i], cieobs=cieobs, relative=False)
elif (inputtype == 'xyz'):
xyz = data[i]
lms = np.dot(_CMF[cieobs]['M'], xyz.T).T # convert to l,m,s
rgb = (lms / _CMF[cieobs]['K']) * k # convert to rho, gamma, beta
# apply von-kries cat with D = 1:
if (rgbb == 0).any():
Mcat = np.eye(3)
else:
Mcat = np.diag((rgbr / rgbb)[0])
rgba = np.dot(Mcat, rgb.T).T
# apply naka-rushton compression:
rgbc = naka_rushton(rgba,
n=naka['n'],
sig=naka['sig'](rgbr.mean()),
noise=naka['noise'],
scaling=naka['scaling'])
#rgbc = np.ones(rgbc.shape)*rgbc.mean() # test if eew ends up at origin
# calculate achromatic and color difference signals, A, a, b:
Aab = np.dot(MAab, rgbc.T).T
A, a, b = asplit(Aab)
a = ca * a
b = cb * b
# calculate colorfullness like signal M:
M = cM * ((a**2.0 + b**2.0)**0.5)
# calculate brightness Q:
Q = cA * (
A + cHK[0] * M**cHK[1]
) # last term is contribution of Helmholtz-Kohlrausch effect on brightness
# calculate saturation, s:
s = M / Q
S = s # make extra variable, jsut in case 'S' is called
# calculate amount of white, W:
W = 1 / (1.0 + cW[0] * (s**cW[1]))
# adjust Q for size (fov) of stimulus (matter of debate whether to do this before or after calculation of s or W, there was no data on s, M or W for different sized stimuli: after)
Q = Q * (fov / 10.0)**cfov
# calculate hue, h and Hue quadrature, H:
h = hue_angle(a, b, htype='deg')
if 'H' in outin:
H = hue_quadrature(h, unique_hue_data=unique_hue_data)
else:
H = None
# calculate cart. co.:
if 'aM' in outin:
aM = M * np.cos(h * np.pi / 180.0)
bM = M * np.sin(h * np.pi / 180.0)
if 'aS' in outin:
aS = s * np.cos(h * np.pi / 180.0)
bS = s * np.sin(h * np.pi / 180.0)
if 'aW' in outin:
aW = W * np.cos(h * np.pi / 180.0)
bW = W * np.sin(h * np.pi / 180.0)
if (outin != ['Q', 'as', 'bs']):
camout[i] = eval('ajoin((' + ','.join(outin) + '))')
else:
camout[i] = ajoin((Q, aS, bS))
elif direction == 'inverse':
# get Q, M and a, b depending on input type:
if 'aW' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
W = (a**2.0 + b**2.0)**0.5
s = (((1.0 / W) - 1.0) / cW[0])**(1.0 / cW[1])
M = s * Q
if 'aM' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
M = (a**2.0 + b**2.0)**0.5
if 'aS' in outin:
Q, a, b = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
s = (a**2.0 + b**2.0)**0.5
M = s * Q
if 'h' in outin:
Q, WsM, h = asplit(data[i])
Q = Q / (
(fov / 10.0)**cfov
) #adjust Q for size (fov) of stimulus back to that 10° ref
if 'W' in outin:
s = (((1.0 / WsM) - 1.0) / cW[0])**(1.0 / cW[1])
M = s * Q
elif 's' in outin:
M = WsM * Q
elif 'M' in outin:
M = WsM
# calculate achromatic signal, A from Q and M:
A = Q / cA - cHK[0] * M**cHK[1]
# calculate hue angle:
h = hue_angle(a, b, htype='rad')
# calculate a,b from M and h:
a = (M / cM) * np.cos(h)
b = (M / cM) * np.sin(h)
a = a / ca
b = b / cb
# create Aab:
Aab = ajoin((A, a, b))
# calculate rgbc:
rgbc = np.dot(invMAab, Aab.T).T
# decompress rgbc to (adapted) rgba :
rgba = naka_rushton(rgbc,
n=naka['n'],
sig=naka['sig'](rgbr.mean()),
noise=naka['noise'],
scaling=naka['scaling'],
direction='inverse')
# apply inverse von-kries cat with D = 1:
rgb = np.dot(np.diag((rgbb / rgbr)[0]), rgba.T).T
# convert rgb to lms to xyz:
lms = rgb / k * _CMF[cieobs]['K']
xyz = np.dot(Mlms2xyz, lms.T).T
camout[i] = xyz
camout = np.transpose(camout, axes=(1, 0, 2))
if camout.shape[1] == 1:
camout = np.squeeze(camout, axis=1)
return camout
