/usr/lib/python2.7/dist-packages/PyMca/EPDL97/EADLParser.py is in pymca 4.7.1+dfsg-2.
This file is owned by root:root, with mode 0o644.
The actual contents of the file can be viewed below.
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import os
__doc__ =\
"""
The 1997 release of the Evaluated Atomic Data Library (EADL97)
This module parses the EADL.DAT file that can be downloaded from:
http://www-nds.iaea.org/epdl97/libsall.htm
EADL contains atomic relaxation information for use in particle transport
analysis for atomic number Z = 1-100 and for each subshell.
The original units are in cm and MeV.
The specific data are:
- Subshell data
a) number of electrons
b) binding and kinetic energy (MeV)
c) average radius (cm)
d) radiative and non-radiative level widths (MeV)
e) average number of released electrons and x-rays
f) average energy of released electrons and x-rays (MeV)
g) average energy to the residual atom, i.e., local deposition (MeV)
- Transition probability data
a) radiation transition probabilities
b) non-radiative transition probabilities
The data are organized in blocks with headers.
The first line of the header:
Columns Format Definition
1-3 I3 Z - atomic number
4-6 I3 A - mass number (in all cases=0 for elemental data)
8-9 I2 Yi - incident particle designator (7 is photon)
11-12 I2 Yo - outgoing particle designator (0, no particle
7, photon
8, positron
9, electron)
14-24 E11.4 AW - atomic mass (amu)
26-31 I6 Date of evaluation (YYMMDD)
The second line of the header:
Columns Format Definition
1-2 I2 C - reaction descriptor
= 71, coherent scattering
= 72, incoherent scattering
= 73, photoelectric effect
= 74, pair production
= 75, triplet production
= 91, subshell parameters
= 92, transition probabilities
= 93, whole atom parameters
3-5 I2 I - reaction property:
= 0, integrated cross section
= 10, avg. energy of Yo
= 11, avg. energy to the residual atom
= 912, number of electrons
= 913, binding energy
= 914, kinetic energy
= 915, average radius
= 921, radiative level width
= 922, non-radiative level width
= 931, radiative transition probability
= 932, non-radiative transition probability
= 933, particles per initial vacancy
= 934, energy of particles per initial vacancy
= 935, average energy to the residual atom, i.e.
local deposition, per initial vacancy
--- moved to EPDL97 ---
= 941, form factor
= 942, scattering function
= 943, imaginary anomalous scatt. factor
= 944, real anomalous scatt. factor
6-8 I3 S - reaction modifier:
= 0 no X1 field data required
= 91 X1 field data required
22-32 #11.4 X1 - subshell designator
0 if S is 0
if S is 91, subshell designator
Summary of the EADL Data Base
--------------------------------------------------------------------------
Yi C S X1 Yo I Data Types
--------------------------------------------------------------------------
Subshell parameters
--------------------------------------------------------------------------
0 91 0 0. 0 912 number of electrons
0 91 0 0. 0 913 binding energy
0 91 0 0. 0 914 kinetic energy
0 91 0 0. 0 915 average radius
0 91 0 0. 0 921 radiative level width
0 91 0 0. 0 921 non-radiative level width
--------------------------------------------------------------------------
Transititon probabilities
--------------------------------------------------------------------------
0 92 0 0. 0 935 average energy to the residual atom
0 92 0 0. 7 or 9 933 average number of particles per
initial vacancy
0 92 0 0. 7 or 9 934 average energy of particles per
initial vacancy
0 92 91 * 0 931 radiative transition probability
0 92 91 * 0 932 non-radiative transition probability
---------------------------------------------------------------------------
Yi C S X1 Yo I Data Types
--------------------------------------------------------------------------
* -> Subshell designator
Data sorted in ascending order Z -> C -> S -> X1 -> Yo -> I
"""
import numpy
#Translation from EADL index to actual shell (Table VI)
import EADLSubshells
SHELL_LIST = EADLSubshells.SHELL_LIST
getSubshellFromValue = EADLSubshells.getSubshellFromValue
getValueFromSubshell = EADLSubshells.getValueFromSubshell
DEBUG = 0
AVOGADRO_NUMBER = 6.02214179E23
#
Elements = ['H', 'He',
'Li', 'Be', 'B', 'C', 'N', 'O', 'F', 'Ne',
'Na', 'Mg', 'Al', 'Si', 'P', 'S', 'Cl', 'Ar',
'K', 'Ca', 'Sc', 'Ti', 'V', 'Cr', 'Mn', 'Fe',
'Co', 'Ni', 'Cu', 'Zn', 'Ga', 'Ge', 'As', 'Se',
'Br', 'Kr', 'Rb', 'Sr', 'Y', 'Zr', 'Nb', 'Mo',
'Tc', 'Ru', 'Rh', 'Pd', 'Ag', 'Cd', 'In', 'Sn',
'Sb', 'Te', 'I', 'Xe', 'Cs', 'Ba', 'La', 'Ce',
'Pr', 'Nd', 'Pm', 'Sm', 'Eu', 'Gd', 'Tb', 'Dy',
'Ho', 'Er', 'Tm', 'Yb', 'Lu', 'Hf', 'Ta', 'W',
'Re', 'Os', 'Ir', 'Pt', 'Au', 'Hg', 'Tl', 'Pb',
'Bi', 'Po', 'At', 'Rn', 'Fr', 'Ra', 'Ac', 'Th',
'Pa', 'U', 'Np', 'Pu', 'Am', 'Cm', 'Bk', 'Cf',
'Es', 'Fm', 'Md', 'No', 'Lr', 'Rf', 'Db', 'Sg',
'Bh', 'Hs', 'Mt']
#Read the EPDL library
# Try to find it in the local directory
EADL = os.path.join(os.path.dirname(__file__), 'EADL.DAT')
if not os.path.exists(EADL):
from PyMca import PyMcaDataDir
EADL = os.path.join(PyMcaDataDir.PYMCA_DATA_DIR, 'EPDL97', 'EADL.DAT')
infile = open(EADL, 'rb')
if sys.version < '3.0':
EADL97_DATA = infile.read()
else:
EADL97_DATA = infile.read().decode('UTF-8')
infile.close()
#speed up sequential access
LAST_INDEX = -1
#properly write exponential notation
#EADL97_DATA = EADL97_DATA.replace('- ', ' ')
#EADL97_DATA = EADL97_DATA.replace('+ ', ' ')
EADL97_DATA = EADL97_DATA.replace('- ', 'E-')
EADL97_DATA = EADL97_DATA.replace('+ ', 'E+')
#get rid of tabs if any
EADL97_DATA = EADL97_DATA.replace('\t', ' ')
#get rid of carriage returns if any
EADL97_DATA = EADL97_DATA.replace('\r\n', '\n')
EADL97_DATA = EADL97_DATA.split('\n')
#Now I have a huge list with all the lines
EADL97_ATOMIC_WEIGHTS = None
def getParticle(value):
"""
Returns one of ['none', 'photon', 'positron', 'electron'] following
the convention:
0 = no particle
7 = photon
8 = positron
9 = electron)
"""
if value == 7:
return 'photon'
if value == 0:
return 'none'
if value == 9:
return 'electron'
if value == 8:
return 'positron'
raise ValueError('Invalid particle code')
def getReactionFromCode(value):
"""
The input value must be one of: 91, 92, 73, 74, 75
Returns one of coherent, incoherent, photoelectric, pair, triplet
according to the integer EADL97 code of the reaction:
91 <-> subshell parameters
92 <-> transition probabilities
93 <-> whole atom parameters
"""
if value == 91:
return 'subshell'
if value == 92:
return 'transition'
raise ValueError('Invalid reaction descriptor code')
def getReactionPropertyFromCode(value):
"""
The input value must be one of: 0, 10, 11, 941, 942, 943, 944
according to the integer EPDL97 code of the reaction property:
0 <-> integrated cross section
10 <-> avg. energy of Yo
11 <-> avg. energy to the residual atom
912 <-> number of electrons
913 <-> binding energy
914 <-> kinetic energy
915 <-> average radius
921 <-> radiative level width
922 <-> non-radiative level width
931 <-> radiative transition probability
932 <-> non-radiative transition probability
934 <-> energy of particles per initial vacancy
935 <-> average energy to the residual atom, i.e.
941 <-> form factor
942 <-> scattering function
943 <-> imaginary anomalous scatt. factor
944 <-> real anomalous scatt. factor
"""
if value == 0:
return 'cross_section'
if value == 10:
return 'secondary_particle_energy'
if value == 11:
return 'atom_energy_transfer'
if value == 912:
return 'number_of_electrons'
if value == 913:
return 'binding_energy'
if value == 914:
return 'kinetic_energy'
if value == 915:
return 'average_radius'
if value == 921:
return 'radiative_level_width'
if value == 922:
return 'non-radiative_level_width'
if value == 931:
return 'radiative_transition_probability'
if value == 932:
return 'non-radiative_transition_probability'
if value == 933:
return 'particles_per_initial_vacancy'
if value == 934:
return 'energy_of_particles_per_initial_vacancy'
if value == 935:
return 'average_energy_to_the_residual_atom'
if value == 941:
return 'form_factor'
if value == 942:
return 'scattering_function'
if value == 943:
return 'imaginary_anomalous_scattering_factor'
if value == 944:
return 'real_anomalous_scattering_factor'
raise ValueError('Invalid reaction property descriptor code')
def parseHeader0(line):
"""
Columns Format Definition
1-3 I3 Z - atomic number
4-6 I3 A - mass number (in all cases=0 for elemental data)
8-9 I2 Yi - incident particle designator (7 is photon)
11-12 I2 Yo - outgoing particle designator (0, no particle
7, photon
8, positron
9, electron)
14-24 E11.4 AW - atomic mass (amu)
26-31 I6 Date of evaluation (YYMMDD)
"""
item0 = line[0:6]
items = line[6:].split()
Z = int(item0[0:3])
A = int(item0[3:6])
Yi = int(items[0])
Yo = int(items[1])
AW = float(items[2])
Date = items[4]
ddict={}
ddict['atomic_number'] = Z
ddict['mass_number'] = A
ddict['atomic_mass'] = AW
ddict['incident_particle'] = getParticle(Yi)
ddict['incident_particle_value'] = Yi
ddict['outgoing_particle'] = getParticle(Yo)
ddict['outgoing_particle_value'] = Yo
ddict['date'] = Date
ddict['Z'] = Z
ddict['A'] = A
ddict['Yi'] = Yi
ddict['Yo'] = Yo
ddict['AW'] = AW
return ddict
def parseHeader1(line):
"""
The second line of the header:
Columns Format Definition
1-2 I2 C - reaction descriptor
= 71, coherent scattering
= 72, incoherent scattering
= 73, photoelectric effect
= 74, pair production
= 75, triplet production
= 91, subshell parameters
= 92, transition probabilities
= 93, whole atom parameters
3-5 I2 I - reaction property:
= 0, integrated cross section
= 10, avg. energy of Yo
= 11, avg. energy to the residual atom
= 912, number of electrons
= 913, binding energy
= 914, kinetic energy
= 915, average radius
= 921, radiative level width
= 922, non-radiative level width
= 931, radiative transition probability
= 932, non-radiative transition probability
= 934, energy of particles per initial vacancy
= 935, average energy to the residual atom, i.e.
local deposition, per initial vacancy
--- moved to EPDL97 ---
= 941, form factor
= 942, scattering function
= 943, imaginary anomalous scatt. factor
= 944, real anomalous scatt. factor
6-8 I3 S - reaction modifier:
= 0 no X1 field data required
= 91 X1 field data required
22-32 #11.4 X1 - subshell designator
0 if S is 0
if S is 91, subshell designator
"""
item0 = line[0:6]
items = line[6:].split()
C = int(item0[0:2])
I = int(item0[2:6])
S = int(items[0])
#there seems to be some dummy number in between
X1 = float(items[2])
ddict={}
ddict['reaction_code'] = C
ddict['reaction'] = getReactionFromCode(C)
ddict['reaction_property'] = getReactionPropertyFromCode(I)
ddict['reaction_property_code'] = I
ddict['C'] = C
ddict['I'] = I
ddict['S'] = S
ddict['X1'] = X1
if S == 91:
ddict['subshell_code'] = X1
if X1 != 0.0:
ddict['subshell'] = getSubshellFromValue(X1)
else:
ddict['subshell'] = 'none'
elif (S == 0) and (X1 == 0.0):
ddict['subshell_code'] = 0
ddict['subshell'] = 'none'
else:
print("Inconsistent data")
print("X1 = ", X1, "S = ", S)
sys.exit(1)
return ddict
def parseHeader(line0, line1):
#print "line0 = ", line0
#print "line1 = ", line1
ddict = parseHeader0(line0)
ddict.update(parseHeader1(line1))
return ddict
if 0:
ddict = parseHeader0(EADL97_DATA[0])
for key in ddict.keys():
print(key, ddict[key])
if 0:
ddict = parseHeader1(EADL97_DATA[1])
for key in ddict.keys():
print(key, ddict[key])
def getDataLineIndex(lines, z, Yi, C, S, X1, Yo, I):
global LAST_INDEX
if (z < 1) or (z>100):
raise ValueError("Invalid atomic number %d" % z)
nlines = len(lines)
i = LAST_INDEX
while i < (nlines-1):
i += 1
line = lines[i]
if len(line.split()) < 9:
"""
i += 2
while len(lines[i+1].split()) != 1:
print lines[i+1]
if i>=5:
sys.exit(0)
i += 1
"""
continue
try:
ddict = parseHeader(lines[i], lines[i+1])
except:
print("Error with lines")
print("line index = %d" % i)
print(lines[i])
print(lines[i+1])
print(sys.exc_info())
raise
if 0:
print(ddict['Z'], z)
print(ddict['Yi'], Yi)
print(ddict['C'], C)
print(ddict['S'], S)
print(ddict['X1'], X1)
print(ddict['Yo'], Yo)
print(ddict['I'], I)
if DEBUG:
if ddict['Z'] == z:
print("Z found")
if ddict['Yi'] == Yi:
print("Yi found")
if ddict['C'] == C:
print("C found")
if ddict['S'] == S:
print("S found with X1 = ", ddict['X1'])
print("Requested X1 = ", X1)
print(lines[i])
print(lines[i+1])
if ddict['X1'] == X1:
print("Requested Yo = ", Yo)
print("Found Yo = ", ddict['Yo'])
if ddict['Yo'] == Yo:
print("Requested I = ",I)
if ddict['I'] == I:
print("FOUND!")
print(lines[i])
print(lines[i+1])
LAST_INDEX = i - 1
return i
break
else:
if ddict['Z'] == z:
if ddict['Yi'] == Yi:
if ddict['C'] == C:
if ddict['S'] == S:
if ddict['X1'] == X1:
if ddict['Yo'] == Yo:
if ddict['I'] == I:
LAST_INDEX = i - 1
return i
break
i += 1
if LAST_INDEX > 0:
if DEBUG:
print("REPEATING")
LAST_INDEX = -1
return getDataLineIndex(lines, z, Yi, C, S, X1, Yo, I)
return -1
def getActualDataFromLinesAndOffset(lines, index):
data_begin = index + 2
data_end = index + 2
end_line = lines[data_end+1]
while (len(end_line) != 72) and (end_line[-1] != '1'):
data_end += 1
end_line = lines[data_end + 1]
data_end += 1
if DEBUG:
print("COMPLETE DATA SET")
print(lines[index:data_end])
print("END DATA SET")
print("ADDITIONAL LINE")
print(lines[data_end])
print("END ADDITIONAL LINE")
ndata = data_end - data_begin
energy = numpy.zeros((ndata,), numpy.float)
t = lines[data_begin].split()
if len(t) == 2:
value = numpy.zeros((ndata,), numpy.float)
for i in range(ndata):
t = lines[data_begin+i].split()
energy[i] = float(t[0])
try:
value[i] = float(t[1])
except ValueError:
if ('E' not in t[1]) and (('+' in t[1]) or ('-' in t[1])):
t[1] = t[1].replace('-','E-')
t[1] = t[1].replace('+','E+')
value[i] = float(t[1])
else:
raise
else:
value = []
for i in range(ndata):
t = lines[data_begin+i].split()
energy[i] = float(t[0])
value.append([])
for j in range(0, len(t)-1):
tj = t[j+1]
try:
value[i].append(float(tj))
except ValueError:
if ('E' not in tj) and (('+' in tj) or ('-' in tj)):
tj = tj.replace('-','E-')
tj = tj.replace('+','E+')
value[i].append(float(tj))
else:
raise
return energy, value
def getBaseShellDict(nvalues=None):
bad_shells = ['L (', 'L23',
'M (', 'M23', 'M45',
'N (', 'N23', 'N45', 'N67',
'O (', 'O23', 'O45', 'O67', 'O89',
'P (', 'P23', 'P45', 'P67', 'P89', 'P101',
'Q (', 'Q23', 'Q45', 'Q67']
ddict = {}
for shell in SHELL_LIST:
if shell[0:3] in bad_shells:
continue
if shell[0:4] in bad_shells:
continue
if nvalues is None:
ddict[shell] = 0.0
else:
ddict[shell] = [0.0] * nvalues
return ddict
def getBaseShellList():
bad_shells = ['L (', 'L23',
'M (', 'M23', 'M45',
'N (', 'N23', 'N45', 'N67',
'O (', 'O23', 'O45', 'O67', 'O89',
'P (', 'P23', 'P45', 'P67', 'P89', 'P101',
'Q (', 'Q23', 'Q45', 'Q67']
ddict = []
for shell in SHELL_LIST:
if shell[0:3] in bad_shells:
continue
if shell[0:4] in bad_shells:
continue
ddict.append(shell)
return ddict
def getRadiativeWidths(z, lines=None):
#Yi C S X1 Yo I
#0 91 0 0. 0 921 Radiative widths
ddict = getBaseShellDict()
if z < 6:
return ddict
if lines is None:
lines = EADL97_DATA
index = getDataLineIndex(lines, z, 0, 91, 0, 0., 0, 921)
if index < 0:
raise IOError("Requested data not found")
shell_codes, value = getActualDataFromLinesAndOffset(lines, index)
if DEBUG:
print("shell_codes, value ",shell_codes, value)
i = 0
ddict = getBaseShellDict()
for code in shell_codes:
shell = getSubshellFromValue(code)
ddict[shell] = value[i]
i += 1
return ddict
def getNonradiativeWidths(z, lines=None):
#Yi C S X1 Yo I
#0 91 0 0. 0 922 Nonradiative widths
ddict = getBaseShellDict()
if z < 6:
return ddict
if lines is None:
lines = EADL97_DATA
index = getDataLineIndex(lines, z, 0, 91, 0, 0., 0, 922)
if index < 0:
raise IOError("Requested data not found")
shell_codes, value = getActualDataFromLinesAndOffset(lines, index)
if DEBUG:
print("shell_codes, value ",shell_codes, value)
i = 0
ddict = getBaseShellDict()
for code in shell_codes:
shell = getSubshellFromValue(code)
ddict[shell] = value[i]
i += 1
return ddict
def getRadiativeTransitionProbabilities(z, shell='K', lines=None):
"""
getRadiativeTransitionProbabilities(z, shell='K')
Returns a dictionary with the radiative transition probabilities
from any shell to the given shell.
"""
#Yi C S X1 Yo I
#0 92 91 1. 7 931 K Shell
#0 92 91 2. 7 931 L1 Shell
#0 92 91 5. 7 931 L2 Shell
#0 92 91 6. 7 931 L3 Shell
#0 92 91 8. 7 931 M1 Shell
#0 92 91 10. 7 931 M2 Shell
#0 92 91 11. 7 931 M3 Shell
#0 92 91 13. 7 931 M4 Shell
#0 92 91 14. 7 931 M5 Shell
ddict = getBaseShellDict(nvalues=2)
if z < 6:
return ddict
if lines is None:
lines = EADL97_DATA
X1 = getValueFromSubshell(shell)
index = getDataLineIndex(lines, z, 0, 92, 91, X1, 7, 931)
if index < 0:
#this error may happen when requesting non existing data too
raise IOError("Requested data not found")
shell_codes, values = getActualDataFromLinesAndOffset(lines, index)
if DEBUG:
print("shell_codes, values ",shell_codes, values)
i = 0
ddict = getBaseShellDict(nvalues=2)
for code in shell_codes:
key = getSubshellFromValue(code)
ddict[key] = values[i]
i += 1
return ddict
def getNonradiativeTransitionProbabilities(z, shell='K', lines=None):
"""
getNonradiativeTransitionProbabilities(z, shell='K')
Returns the radiative transition probabilities and energies
to the given shell.
The output is a dictionary in IUPAC notation.
"""
#Yi C S X1 Yo I
#0 92 91 1. 9 932 K Shell
#0 92 91 2. 9 932 L1 Shell
#0 92 91 5. 9 932 L2 Shell
#0 92 91 6. 9 932 L3 Shell
#0 92 91 8. 9 932 M1 Shell
#0 92 91 10. 9 932 M2 Shell
#0 92 91 11. 9 932 M3 Shell
#0 92 91 13. 9 932 M4 Shell
#0 92 91 14. 9 932 M5 Shell
ddict = getBaseShellDict()
#if z < 6:
# return ddict
if lines is None:
lines = EADL97_DATA
X1 = getValueFromSubshell(shell)
index = getDataLineIndex(lines, z, 0, 92, 91, X1, 9, 932)
if index < 0:
#this error may happen when requesting non existing data too
raise IOError("Requested data not found")
shell_codes, values = getActualDataFromLinesAndOffset(lines, index)
if DEBUG:
print("shell_codes, values ",shell_codes, values)
i = 0
ddict = {}#getBaseShellDict()
for code in shell_codes:
key1 = getSubshellFromValue(code).split()[0]
key2 = getSubshellFromValue(values[i][0]).split()[0]
ddict[shell+'-'+key1+key2] = values[i][1:]
i += 1
return ddict
#The usefull stuff
def getBindingEnergies(z, lines=None):
"""
getBindingEnergies(z)
Returns the binding energies in MeV
"""
#Yi C S X1 Yo I
#0 91 0 0. 0 913
if lines is None:
lines = EADL97_DATA
index = getDataLineIndex(lines, z, 0, 91, 0, 0., 0, 913)
if index < 0:
raise IOError("Requested data not found")
shell_codes, value = getActualDataFromLinesAndOffset(lines, index)
if DEBUG:
print("shell_codes, value ",shell_codes, value)
i = 0
ddict = getBaseShellDict()
for code in shell_codes:
shell = getSubshellFromValue(code)
ddict[shell] = value[i]
i += 1
return ddict
def getFluorescenceYields(z, lines=None):
if lines is None:
lines = EADL97_DATA
radiative_dict = getRadiativeWidths(z, lines)
nonradiative_dict = getNonradiativeWidths(z, lines)
ddict={}
for key in radiative_dict.keys():
x = radiative_dict[key]
a = nonradiative_dict[key]
if ( x > 0.0) or ( a > 0.0):
ddict[key] = x / (a + x)
return ddict
def getCosterKronigYields(z, shell='L1', lines=None):
"""
getCosterKronigYields(z, shell='L1')
Returns the non-zero Coster-Kronig yields as keys of a dictionnary
or just an empty dictionnary.
"""
if lines is None:
lines = EADL97_DATA
#radiative_dict = getRadiativeWidths(z, lines)
#nonradiative_dict = getNonradiativeWidths(z, lines)
probabilities = getNonradiativeTransitionProbabilities(z,
shell=shell,
lines=lines)
ddict = {}
for key in probabilities:
items = key.split('-')
if items[0] != shell:
raise ValueError("Inconsistent data!")
if items[0][0] == items[1][0]:
#coster kronig
transition = 'f'+ items[0][1] + items[1][1]
if transition not in ddict.keys():
ddict[transition] = 0.0
ddict[transition] += probabilities[key][0]
return ddict
def getLShellCosterKronigYields(z, lines=None):
"""
getLShellCosterKronigYields(z)
Returns the L-shell Coster-Kronig yields of an element as keys of a
dictionnary
"""
ddict = {}
ddict['f12'] = 0.0
ddict['f13'] = 0.0
ddict['f23'] = 0.0
for i in range(2):
shell = 'L%d' % (i+1)
try:
ddict.update(getCosterKronigYields(z, shell=shell))
except IOError:
pass
return ddict
def getMShellCosterKronigYields(z, lines=None):
"""
getMShellCosterKronigYields(z)
Returns the M-shell Coster-Kronig yields of an element as keys of a
dictionnary. It does not check for physical meaning. So, it will give
zeroes when needed.
"""
ddict = {}
for i in range(1, 5):
for j in range(i+1, 6):
key = 'f%d%d' % (i,j)
ddict[key] = 0.0
shell = 'M%d' % i
try:
ddict.update(getCosterKronigYields(z, shell=shell))
except IOError:
pass
return ddict
def getAtomicWeights():
global EADL97_ATOMIC_WEIGHTS
if EADL97_ATOMIC_WEIGHTS is None:
lines = EADL97_DATA
i = 1
EADL97_ATOMIC_WEIGHTS = numpy.zeros((len(Elements),), numpy.float)
for line in lines:
if line.startswith('%3d000 ' % i):
ddict0 = parseHeader0(line)
EADL97_ATOMIC_WEIGHTS[i-1] = ddict0['atomic_mass']
i += 1
return EADL97_ATOMIC_WEIGHTS * 1
if __name__ == "__main__":
if len(sys.argv) > 1:
element = sys.argv[1]
else:
element = 'Pb'
print("Getting binding energies for element %s" % element)
ddict = getBindingEnergies(Elements.index(element)+1)
for key in getBaseShellList():
if ddict[key] > 0.0:
print("Shell = %s Energy (keV) = %.7E" % (key, ddict[key] * 1000.))
print("Getting fluorescence yields for element %s" % element)
ddict = getFluorescenceYields(Elements.index(element)+1)
for key in getBaseShellList():
if key in ddict:
if ddict[key] > 0.0:
print("Shell = %s Yield = %.7E" % (key, ddict[key]))
#total_emission = 0.0
for shell in ['K', 'L1', 'L2', 'L3', 'M1', 'M2', 'M3', 'M4', 'M5']:
try:
ddict = getRadiativeTransitionProbabilities(Elements.index(element)+1,
shell=shell)
print("%s Shell radiative emission probabilities " % shell)
except IOError:
continue
total = 0.0
for key in getBaseShellList():
if key in ddict:
if ddict[key][0] > 0.0:
print("Shell = %s Yield = %.7E Energy = %.7E" % (key, ddict[key][0],
ddict[key][1] * 1000.))
total += ddict[key][0]
print("Total %s-shell emission probability = %.7E" % (shell, total))
#total_emission += total
#print "total_emission = ", total_emission
for shell in ['K', 'L1', 'L2', 'L3', 'M1', 'M2', 'M3', 'M4', 'M5']:
try:
ddict = getNonradiativeTransitionProbabilities(Elements.index(element)+1,
shell=shell)
print("%s Shell Nonradiative emission probabilities " % shell)
except IOError:
continue
total = 0.0
shell_list = getBaseShellList()
for key0 in shell_list:
for key1 in shell_list:
key = "%s-%s%s" % (shell, key0.split()[0], key1.split()[0])
if key in ddict:
if ddict[key][0] > 0.0:
print("Shell = %s Yield = %.7E Energy = %.7E" %\
(key, ddict[key][0], ddict[key][1] * 1000.))
total += ddict[key][0]
print("Total %s-shell non-radiative emission probability = %.7E" % (shell, total))
if shell in ['K']:
for key0 in ['L1', 'L2' ,'L3']:
subtotal = 0.0
for key1 in shell_list:
tmpKey = key1.split()[0]
key = "%s-%s%s" % (shell, key0, tmpKey)
if key in ddict:
if ddict[key][0] > 0.0:
subtotal += ddict[key][0]
if tmpKey == key0:
subtotal += ddict[key][0]
print("%s vacancies for nonradiative transition to %s shell = %.7E"%\
(key0, shell, subtotal))
#print(getNonradiativeTransitionProbabilities(Elements.index(element)+1, 'L1'))
print(getMShellCosterKronigYields(Elements.index(element)+1))
print("atomic weight = ", getAtomicWeights()[Elements.index(element)])
sys.exit(0)
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