/usr/share/pymca/LShellRatesCampbell.dat is in pymca-data 4.7.1+dfsg-2.
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1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 293 294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324 325 326 327 328 329 330 331 332 333 334 335 336 337 338 339 340 341 342 343 344 345 346 347 348 349 350 351 352 353 354 355 356 357 358 359 360 361 362 | #S 1 L1 Subshell X-ray emission rates.
#U0 File: AP0L1R.DAT received by courtesy of J.L. Campbell
#U1
#U2 X-ray emission rates for determining relative x-ray line intensities.
#U3
#U4 Reference: J.L.Campbell and J.X.Wang. Interpolated Dirac-Fock values of L
#U5 subshell X-ray emission rates including overlap and exchange effects. At.Data
#U6 Nucl.Data Tables 43 (1989) 281-291.
#U7
#N 10
#L Z L1L3 L1M2 L1M3 L1N2 L1N3 L1O23 L1P23 L1M45 L1N45
1 0 0 0 0 0 0 0 0 0
2 0 0 0 0 0 0 0 0 0
3 0 0 0 0 0 0 0 0 0
4 0 0 0 0 0 0 0 0 0
5 0 0 0 0 0 0 0 0 0
6 0 0 0 0 0 0 0 0 0
7 0 0 0 0 0 0 0 0 0
8 0 0 0 0 0 0 0 0 0
9 0 0 0 0 0 0 0 0 0
10 0 0 0 0 0 0 0 0 0
11 0 0 0 0 0 0 0 0 0
12 0 0 0 0 0 0 0 0 0
13 0 0 0 0 0 0 0 0 0
14 0 0 0 0 0 0 0 0 0
15 0 0 0 0 0 0 0 0 0
16 0 0 0 0 0 0 0 0 0
17 0 0 0 0 0 0 0 0 0
18 8.559E-2 3.125E-1 6.019E-1 0 0 0 0 0 0
19 6.223E-2 3.205E-1 6.173E-1 0 0 0 0 0 0
20 4.786E-2 3.260E-1 6.261E-1 0 0 0 0 0 0
21 3.998E-2 3.295E-1 6.304E-1 0 0 0 0 8.738E-5 0
22 3.401E-2 3.329E-1 6.329E-1 0 0 0 0 2.113E-4 0
23 2.955E-2 3.350E-1 6.351E-1 0 0 0 0 3.738E-4 0
24 2.667E-2 3.365E-1 6.362E-1 0 0 0 0 6.452E-4 0
25 2.331E-2 3.390E-1 6.368E-1 0 0 0 0 8.210E-4 0
26 2.102E-2 3.403E-1 6.375E-1 0 0 0 0 1.108E-3 0
27 1.914E-2 3.419E-1 6.375E-1 0 0 0 0 1.441E-3 0
28 1.757E-2 3.437E-1 6.369E-1 0 0 0 0 1.820E-3 0
29 1.669E-2 3.452E-1 6.358E-1 0 0 0 0 2.337E-3 0
30 1.552E-2 3.465E-1 6.352E-1 0 0 0 0 2.714E-3 0
31 1.448E-2 3.479E-1 6.345E-1 0 0 0 0 3.092E-3 0
32 1.326E-2 3.411E-1 6.187E-1 8.346E-3 1.523E-2 0 0 3.372E-3 0
33 1.227E-2 3.362E-1 6.068E-1 1.454E-2 2.652E-2 0 0 3.683E-3 0
34 1.139E-2 3.298E-1 5.950E-1 2.121E-2 3.852E-2 0 0 3.982E-3 0
35 1.064E-2 3.246E-1 5.817E-1 2.807E-2 5.076E-2 0 0 4.265E-3 0
36 9.979E-3 3.189E-1 5.685E-1 3.509E-2 6.301E-2 0 0 4.528E-3 0
37 9.460E-3 3.151E-1 5.588E-1 3.995E-2 7.188E-2 0 0 4.824E-3 0
38 9.045E-3 3.129E-1 5.507E-1 4.376E-2 7.844E-2 0 0 5.128E-3 0
39 8.727E-3 3.117E-1 5.458E-1 4.611E-2 8.219E-2 0 0 5.458E-3 0
40 8.475E-3 3.113E-1 5.412E-1 4.805E-2 8.518E-2 0 0 5.791E-3 6.392E-5
41 8.304E-3 3.117E-1 5.382E-1 4.913E-2 8.644E-2 0 0 6.155E-3 1.358E-4
42 8.143E-3 3.112E-1 5.345E-1 5.074E-2 8.878E-2 0 0 6.504E-3 1.981E-4
43 8.032E-3 3.113E-1 5.304E-1 5.226E-2 9.091E-2 0 0 6.860E-3 2.707E-4
44 7.964E-3 3.112E-1 5.268E-1 5.367E-2 9.279E-2 0 0 7.222E-3 3.537E-4
45 7.920E-3 3.113E-1 5.230E-1 5.498E-2 9.474E-2 0 0 7.598E-3 4.475E-4
46 7.915E-3 3.117E-1 5.206E-1 5.582E-2 9.543E-2 0 0 7.988E-3 5.702E-4
47 7.938E-3 3.113E-1 5.164E-1 5.755E-2 9.777E-2 0 0 8.372E-3 6.687E-4
48 7.983E-3 3.108E-1 5.122E-1 5.934E-2 1.002E-1 0 0 8.753E-3 7.658E-4
49 8.062E-3 3.102E-1 5.077E-1 6.110E-2 1.029E-1 0 0 9.176E-3 8.695E-4
50 8.108E-3 3.076E-1 5.013E-1 6.241E-2 1.049E-1 5.205E-3 0 9.501E-3 9.647E-4
51 8.203E-3 3.064E-1 4.956E-1 6.377E-2 1.059E-1 9.128E-3 0 9.898E-3 1.065E-3
52 8.307E-3 3.047E-1 4.899E-1 6.490E-2 1.073E-1 1.350E-2 0 1.028E-2 1.162E-3
53 8.445E-3 3.032E-1 4.835E-1 6.608E-2 1.086E-1 1.828E-2 0 1.067E-2 1.262E-3
54 8.602E-3 3.017E-1 4.774E-1 6.703E-2 1.096E-1 2.336E-2 0 1.106E-2 1.359E-3
55 8.786E-3 3.008E-1 4.715E-1 6.814E-2 1.107E-1 2.716E-2 0 1.146E-2 1.460E-3
56 8.999E-3 3.001E-1 4.663E-1 6.919E-2 1.117E-1 3.026E-2 0 1.189E-2 1.565E-3
57 9.253E-3 2.997E-1 4.613E-1 7.047E-2 1.129E-1 3.232E-2 0 1.234E-2 1.674E-3
58 9.598E-3 3.019E-1 4.610E-1 7.088E-2 1.125E-1 2.945E-2 0 1.290E-2 1.733E-3
59 9.933E-3 3.032E-1 4.583E-1 7.160E-2 1.127E-1 2.902E-2 0 1.344E-2 1.816E-3
60 1.032E-2 3.044E-1 4.556E-1 7.234E-2 1.128E-1 2.864E-2 0 1.400E-2 1.903E-3
61 1.072E-2 3.056E-1 4.532E-1 7.296E-2 1.127E-1 2.826E-2 0 1.457E-2 1.988E-3
62 1.117E-2 3.070E-1 4.504E-1 7.365E-2 1.127E-1 2.787E-2 0 1.515E-2 2.075E-3
63 1.166E-2 3.085E-1 4.476E-1 7.425E-2 1.126E-1 2.748E-2 0 1.575E-2 2.162E-3
64 1.216E-2 3.091E-1 4.435E-1 7.505E-2 1.126E-1 2.901E-2 0 1.632E-2 2.272E-3
65 1.273E-2 3.118E-1 4.417E-1 7.551E-2 1.121E-1 2.678E-2 0 1.702E-2 2.348E-3
66 1.334E-2 3.131E-1 4.390E-1 7.624E-2 1.119E-1 2.639E-2 0 1.766E-2 2.445E-3
67 1.399E-2 3.147E-1 4.360E-1 7.677E-2 1.116E-1 2.603E-2 0 1.834E-2 2.542E-3
68 1.467E-2 3.165E-1 4.327E-1 7.736E-2 1.114E-1 2.568E-2 0 1.903E-2 2.642E-3
69 1.544E-2 3.181E-1 4.296E-1 7.813E-2 1.110E-1 2.535E-2 0 1.975E-2 2.747E-3
70 1.624E-2 3.199E-1 4.264E-1 7.865E-2 1.105E-1 2.508E-2 0 2.046E-2 2.853E-3
71 1.708E-2 3.211E-1 4.218E-1 7.933E-2 1.103E-1 2.629E-2 0 2.117E-2 2.979E-3
72 1.797E-2 3.218E-1 4.174E-1 8.019E-2 1.101E-1 2.753E-2 0 2.189E-2 3.108E-3
73 1.894E-2 3.228E-1 4.130E-1 8.088E-2 1.098E-1 2.867E-2 0 2.262E-2 3.244E-3
74 1.995E-2 3.242E-1 4.082E-1 8.163E-2 1.095E-1 2.976E-2 0 2.337E-2 3.390E-3
75 2.104E-2 3.253E-1 4.032E-1 8.245E-2 1.094E-1 3.085E-2 0 2.414E-2 3.539E-3
76 2.221E-2 3.271E-1 3.980E-1 8.323E-2 1.091E-1 3.181E-2 0 2.491E-2 3.696E-3
77 2.349E-2 3.278E-1 3.936E-1 8.427E-2 1.090E-1 3.222E-2 0 2.576E-2 3.865E-3
78 2.482E-2 3.289E-1 3.885E-1 8.495E-2 1.086E-1 3.352E-2 0 2.657E-2 4.034E-3
79 2.622E-2 3.306E-1 3.831E-1 8.567E-2 1.082E-1 3.452E-2 0 2.741E-2 4.208E-3
80 2.772E-2 3.320E-1 3.780E-1 8.643E-2 1.077E-1 3.577E-2 0 2.801E-2 4.388E-3
81 2.937E-2 3.330E-1 3.725E-1 8.714E-2 1.072E-1 3.705E-2 0 2.914E-2 4.578E-3
82 3.098E-2 3.338E-1 3.665E-1 8.777E-2 1.066E-1 3.827E-2 1.348E-3 2.998E-2 4.761E-3
83 3.282E-2 3.350E-1 3.602E-1 8.864E-2 1.058E-1 3.932E-2 2.384E-3 3.087E-2 4.965E-3
84 3.467E-2 3.358E-1 3.544E-1 8.937E-2 1.049E-1 4.037E-2 3.566E-3 3.177E-2 5.170E-3
85 3.677E-2 3.371E-1 3.479E-1 9.000E-2 1.040E-1 4.129E-2 4.853E-3 3.263E-2 5.378E-3
86 3.891E-2 3.381E-1 3.414E-1 9.081E-2 1.031E-1 4.221E-2 6.237E-3 3.362E-2 5.591E-3
87 4.122E-2 3.390E-1 3.352E-1 9.166E-2 1.022E-1 4.315E-2 7.208E-3 3.459E-2 5.821E-3
88 4.363E-2 3.404E-1 3.288E-1 9.240E-2 1.012E-1 4.401E-2 7.974E-3 3.558E-2 6.057E-3
89 4.625E-2 3.418E-1 3.223E-1 9.317E-2 1.002E-1 4.486E-2 8.554E-3 3.661E-2 6.299E-3
90 4.904E-2 3.430E-1 3.158E-1 9.404E-2 9.912E-2 4.577E-2 9.082E-3 3.762E-2 6.553E-3
91 5.201E-2 3.448E-1 3.098E-1 9.494E-2 9.807E-2 4.623E-2 8.658E-3 3.873E-2 6.821E-3
92 5.517E-2 3.467E-1 3.031E-1 9.571E-2 9.693E-2 4.682E-2 8.692E-3 3.986E-2 7.092E-3
93 5.857E-2 3.481E-1 2.962E-1 9.653E-2 9.591E-2 4.734E-2 9.005E-3 4.102E-2 7.379E-3
94 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
95 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
96 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
97 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
98 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
99 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
100 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
101 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
102 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
103 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
104 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
105 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
106 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
107 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
108 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
109 6.215E-2 3.500E-1 2.894E-1 9.730E-2 9.462E-2 4.782E-2 8.834E-3 4.216E-2 7.670E-3
#S 2 L2 Subshell X-ray emission rates.
#U0 File: AP0L2R.DAT received by courtesy of J.L. Campbell
#U1
#U2 X-ray emission rates for determining relative x-ray line intensities.
#U3
#U4 Reference: J.L.Campbell and J.X.Wang. Interpolated Dirac-Fock values of L
#U5 subshell X-ray emission rates including overlap and exchange effects. At.Data
#U6 Nucl.Data Tables 43 (1989) 281-291.
#U7
#N 8
#L Z L2M1 L2M4 L2N1 L2N4 L2O1 L2O4 L2P1
1 0 0 0 0 0 0 0
2 0 0 0 0 0 0 0
3 0 0 0 0 0 0 0
4 0 0 0 0 0 0 0
5 0 0 0 0 0 0 0
6 0 0 0 0 0 0 0
7 0 0 0 0 0 0 0
8 0 0 0 0 0 0 0
9 0 0 0 0 0 0 0
10 0 0 0 0 0 0 0
11 0 0 0 0 0 0 0
12 0 0 0 0 0 0 0
13 0 0 0 0 0 0 0
14 0 0 0 0 0 0 0
15 0 0 0 0 0 0 0
16 0 0 0 0 0 0 0
17 0 0 0 0 0 0 0
18 1 0 0 0 0 0 0
19 1 0 0 0 0 0 0
20 1 0 0 0 0 0 0
21 1 0 0 0 0 0 0
22 1 0 0 0 0 0 0
23 1 0 0 0 0 0 0
24 1 0 0 0 0 0 0
25 1 0 0 0 0 0 0
26 8.246E-2 9.103E-1 7.201E-3 0 0 0 0
27 6.939E-2 9.248E-1 5.859E-3 0 0 0 0
28 5.949E-2 9.358E-1 4.745E-3 0 0 0 0
29 5.044E-2 9.481E-1 1.433E-3 0 0 0 0
30 4.609E-2 9.507E-1 3.200E-3 0 0 0 0
31 4.277E-2 9.535E-1 3.745E-3 0 0 0 0
32 4.033E-2 9.557E-1 3.967E-3 0 0 0 0
33 3.837E-2 9.575E-1 4.108E-3 0 0 0 0
34 3.684E-2 9.589E-1 4.226E-3 0 0 0 0
35 3.556E-2 9.601E-1 4.358E-3 0 0 0 0
36 3.451E-2 9.610E-1 4.489E-3 0 0 0 0
37 3.355E-2 9.617E-1 4.797E-3 0 0 0 0
38 3.271E-2 9.622E-1 5.060E-3 0 0 0 0
39 3.195E-2 9.629E-1 5.151E-3 0 0 0 0
40 3.078E-2 9.492E-1 4.977E-3 1.503E-2 0 0 0
41 2.978E-2 9.356E-1 5.005E-3 2.899E-2 5.843E-4 0 0
42 2.905E-2 9.266E-1 5.066E-3 3.901E-2 2.411E-4 0 0
43 2.829E-2 9.170E-1 5.076E-3 4.935E-2 2.353E-4 0 0
44 2.758E-2 9.073E-1 5.066E-3 5.985E-2 2.266E-4 0 0
45 2.708E-2 8.969E-1 5.067E-3 7.074E-2 2.182E-4 0 0
46 2.646E-2 8.841E-1 4.999E-3 8.418E-2 2.071E-4 0 0
47 2.606E-2 8.758E-1 5.019E-3 9.295E-2 2.144E-4 0 0
48 2.567E-2 8.681E-1 5.036E-3 1.006E-1 5.098E-4 0 0
49 2.526E-2 8.611E-1 5.063E-3 1.080E-1 5.971E-4 0 0
50 2.493E-2 8.546E-1 5.113E-3 1.147E-1 6.448E-4 0 0
51 2.455E-2 8.491E-1 5.156E-3 1.205E-1 6.840E-4 0 0
52 2.426E-2 8.439E-1 5.203E-3 1.259E-1 7.266E-4 0 0
53 2.398E-2 8.391E-1 5.240E-3 1.309E-1 7.786E-4 0 0
54 2.373E-2 8.348E-1 5.277E-3 1.353E-1 8.440E-4 0 0
55 2.349E-2 8.306E-1 5.319E-3 1.397E-1 9.086E-4 0 0
56 2.325E-2 8.262E-1 5.356E-3 1.441E-1 9.706E-4 0 1.592E-4
57 2.299E-2 8.228E-1 5.380E-3 1.477E-1 1.016E-3 0 1.768E-4
58 2.292E-2 8.241E-1 5.368E-3 1.465E-1 9.519E-4 0 1.444E-4
59 2.286E-2 8.229E-1 5.389E-3 1.477E-1 9.428E-4 0 1.382E-4
60 2.275E-2 8.222E-1 5.391E-3 1.486E-1 9.350E-4 0 1.325E-4
61 2.271E-2 8.215E-1 5.401E-3 1.493E-1 9.261E-4 0 1.275E-4
62 2.261E-2 8.209E-1 5.399E-3 1.501E-1 9.171E-4 0 1.231E-4
63 2.253E-2 8.206E-1 5.398E-3 1.505E-1 9.091E-4 0 1.191E-4
64 2.244E-2 8.186E-1 5.421E-3 1.524E-1 9.444E-4 0 1.359E-4
65 2.241E-2 8.195E-1 5.406E-3 1.517E-1 8.949E-4 0 1.124E-4
66 2.237E-2 8.190E-1 5.422E-3 1.522E-1 8.878E-4 0 1.094E-4
67 2.237E-2 8.183E-1 5.426E-3 1.529E-1 8.822E-4 0 1.068E-4
68 2.230E-2 8.180E-1 5.426E-3 1.533E-1 8.755E-4 0 1.039E-4
69 2.230E-2 8.172E-1 5.444E-3 1.540E-1 8.697E-4 0 1.013E-4
70 2.228E-2 8.168E-1 5.447E-3 1.545E-1 8.628E-4 0 9.834E-5
71 2.223E-2 8.155E-1 5.456E-3 1.558E-1 8.908E-4 0 1.101E-4
72 2.219E-2 8.139E-1 5.484E-3 1.574E-1 9.210E-4 0 1.160E-4
73 2.207E-2 8.094E-1 5.476E-3 1.584E-1 9.466E-4 3.552E-3 1.194E-4
74 2.204E-2 8.062E-1 5.497E-3 1.599E-1 9.771E-4 5.281E-3 1.221E-4
75 2.195E-2 8.032E-1 5.508E-3 1.610E-1 1.007E-3 7.192E-3 1.242E-4
76 2.188E-2 7.998E-1 5.525E-3 1.623E-1 1.039E-3 9.291E-3 1.258E-4
77 2.178E-2 7.953E-1 5.532E-3 1.632E-1 1.063E-3 1.313E-2 0
78 2.175E-2 7.927E-1 5.559E-3 1.640E-1 1.092E-3 1.485E-2 5.624E-5
79 2.168E-2 7.893E-1 5.581E-3 1.649E-1 1.118E-3 1.741E-2 5.656E-5
80 2.166E-2 7.867E-1 5.597E-3 1.656E-1 1.149E-3 1.915E-2 1.296E-4
81 2.165E-2 7.836E-1 5.621E-3 1.668E-1 1.179E-3 2.098E-2 1.577E-4
82 2.160E-2 7.809E-1 5.649E-3 1.678E-1 1.211E-3 2.273E-2 1.788E-4
83 2.160E-2 7.781E-1 5.672E-3 1.688E-1 1.239E-3 2.436E-2 1.967E-4
84 2.153E-2 7.756E-1 5.701E-3 1.698E-1 1.270E-3 2.590E-2 2.133E-4
85 2.154E-2 7.728E-1 5.725E-3 1.710E-1 1.301E-3 2.741E-2 2.289E-4
86 2.154E-2 7.702E-1 5.755E-3 1.721E-1 1.333E-3 2.883E-2 2.434E-4
87 2.155E-2 7.676E-1 5.789E-3 1.732E-1 1.365E-3 3.027E-2 2.645E-4
88 2.153E-2 7.651E-1 5.817E-3 1.742E-1 1.395E-3 3.168E-2 2.846E-4
89 2.155E-2 7.623E-1 5.851E-3 1.755E-1 1.425E-3 3.305E-2 3.026E-4
90 2.156E-2 7.599E-1 5.879E-3 1.765E-1 1.454E-3 3.438E-2 3.193E-4
91 2.157E-2 7.579E-1 5.911E-3 1.778E-1 1.478E-3 3.504E-2 3.151E-4
92 2.160E-2 7.558E-1 5.945E-3 1.789E-1 1.507E-3 3.592E-2 3.219E-4
93 2.163E-2 7.537E-1 5.977E-3 1.801E-1 1.533E-3 3.678E-2 3.324E-4
94 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
95 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
96 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
97 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
98 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
99 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
100 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
101 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
102 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
103 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
104 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
105 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
106 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
107 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
108 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
109 2.169E-2 7.519E-1 6.010E-3 1.811E-1 1.557E-3 3.738E-2 3.333E-4
#S 3 L3 Subshell X-ray emission rates.
#U0 File: AP0L3R.DAT received by courtesy of J.L. Campbell
#U1
#U2 X-ray emission rates for determining relative x-ray line intensities.
#U3
#U4 Reference: J.L.Campbell and J.X.Wang. Interpolated Dirac-Fock values of L
#U5 subshell X-ray emission rates including overlap and exchange effects. At.Data
#U6 Nucl.Data Tables 43 (1989) 281-291.
#U7
#N 10
#L Z L3M1 L3M4 L3M5 L3N1 L3N4 L3N5 L3O1 L3O45 L3P1
1 0 0 0 0 0 0 0 0 0
2 0 0 0 0 0 0 0 0 0
3 0 0 0 0 0 0 0 0 0
4 0 0 0 0 0 0 0 0 0
5 0 0 0 0 0 0 0 0 0
6 0 0 0 0 0 0 0 0 0
7 0 0 0 0 0 0 0 0 0
8 0 0 0 0 0 0 0 0 0
9 0 0 0 0 0 0 0 0 0
10 0 0 0 0 0 0 0 0 0
11 0 0 0 0 0 0 0 0 0
12 0 0 0 0 0 0 0 0 0
13 0 0 0 0 0 0 0 0 0
14 0 0 0 0 0 0 0 0 0
15 0 0 0 0 0 0 0 0 0
16 0 0 0 0 0 0 0 0 0
17 0 0 0 0 0 0 0 0 0
18 1 0 0 0 0 0 0 0 0
19 1 0 0 0 0 0 0 0 0
20 1 0 0 0 0 0 0 0 0
21 1 0 0 0 0 0 0 0 0
22 1 0 0 0 0 0 0 0 0
23 1 0 0 0 0 0 0 0 0
24 1 0 0 0 0 0 0 0 0
25 1 0 0 0 0 0 0 0 0
26 8.581E-2 9.302E-2 8.137E-1 7.437E-3 0 0 0 0 0
27 7.263E-2 9.457E-2 8.268E-1 6.042E-3 0 0 0 0 0
28 6.288E-2 9.575E-2 8.364E-1 4.982E-3 0 0 0 0 0
29 5.377E-2 9.734E-2 8.474E-1 1.535E-3 0 0 0 0 0
30 4.935E-2 9.732E-2 8.499E-1 3.474E-3 0 0 0 0 0
31 4.616E-2 9.740E-2 8.524E-1 4.072E-3 0 0 0 0 0
32 4.384E-2 9.744E-2 8.545E-1 4.251E-3 0 0 0 0 0
33 4.204E-2 9.758E-2 8.559E-1 4.523E-3 0 0 0 0 0
34 4.067E-2 9.760E-2 8.570E-1 4.720E-3 0 0 0 0 0
35 3.954E-2 9.762E-2 8.580E-1 4.879E-3 0 0 0 0 0
36 3.865E-2 9.762E-2 8.587E-1 5.003E-3 0 0 0 0 0
37 3.789E-2 9.755E-2 8.593E-1 5.304E-3 0 0 0 0 0
38 3.722E-2 9.762E-2 8.596E-1 5.569E-3 0 0 0 0 0
39 3.665E-2 9.758E-2 8.601E-1 5.714E-3 0 0 0 0 0
40 3.569E-2 9.607E-2 8.468E-1 5.723E-3 1.515E-3 1.341E-2 7.861E-4 0 0
41 3.490E-2 9.471E-2 8.356E-1 5.767E-3 2.925E-3 2.578E-2 3.226E-4 0 0
42 3.429E-2 9.381E-2 8.272E-1 5.884E-3 3.924E-3 3.461E-2 3.170E-4 0 0
43 3.372E-2 9.283E-2 8.185E-1 5.965E-3 4.954E-3 4.370E-2 3.081E-4 0 0
44 3.320E-2 9.182E-2 8.097E-1 6.039E-3 5.999E-3 5.293E-2 3.003E-4 0 0
45 3.293E-2 9.084E-2 8.001E-1 6.089E-3 7.100E-3 6.265E-2 2.909E-4 0 0
46 3.263E-2 8.961E-2 7.892E-1 6.091E-3 8.442E-3 7.400E-2 0 0 0
47 3.237E-2 8.862E-2 7.815E-1 6.163E-3 9.295E-3 8.181E-2 2.635E-4 0 0
48 3.213E-2 8.780E-2 7.746E-1 6.235E-3 1.002E-2 8.859E-2 6.283E-4 0 0
49 3.199E-2 8.704E-2 7.680E-1 6.345E-3 1.074E-2 9.513E-2 7.559E-4 0 0
50 3.183E-2 8.632E-2 7.624E-1 6.467E-3 1.137E-2 1.009E-1 8.068E-4 0 0
51 3.171E-2 8.564E-2 7.573E-1 6.576E-3 1.192E-2 1.060E-1 8.927E-4 0 0
52 3.165E-2 8.514E-2 7.525E-1 6.697E-3 1.243E-2 1.106E-1 9.687E-4 0 0
53 3.158E-2 8.457E-2 7.482E-1 6.818E-3 1.289E-2 1.149E-1 1.036E-3 0 0
54 3.158E-2 8.412E-2 7.442E-1 6.946E-3 1.331E-2 1.187E-1 1.100E-3 0 0
55 3.162E-2 8.378E-2 7.403E-1 7.065E-3 1.370E-2 1.224E-1 1.200E-3 0 0
56 3.169E-2 8.346E-2 7.362E-1 7.176E-3 1.409E-2 1.259E-1 1.301E-3 0 2.123E-4
57 3.175E-2 8.305E-2 7.326E-1 7.300E-3 1.444E-2 1.293E-1 1.381E-3 0 2.383E-4
58 3.205E-2 8.335E-2 7.335E-1 7.356E-3 1.432E-2 1.279E-1 1.304E-3 0 1.971E-4
59 3.227E-2 8.328E-2 7.324E-1 7.446E-3 1.441E-2 1.287E-1 1.305E-3 0 1.903E-4
60 3.246E-2 8.288E-2 7.322E-1 7.528E-3 1.443E-2 1.290E-1 1.301E-3 0 1.842E-4
61 3.275E-2 8.280E-2 7.314E-1 7.612E-3 1.449E-2 1.295E-1 1.302E-3 0 1.794E-4
62 3.308E-2 8.293E-2 7.304E-1 7.727E-3 1.453E-2 1.299E-1 1.306E-3 0 1.753E-4
63 3.333E-2 8.261E-2 7.302E-1 7.796E-3 1.454E-2 1.301E-1 1.306E-3 0 1.710E-4
64 3.360E-2 8.259E-2 7.282E-1 7.914E-3 1.469E-2 1.315E-1 1.371E-3 0 1.970E-4
65 3.399E-2 8.263E-2 7.287E-1 7.995E-3 1.461E-2 1.306E-1 1.316E-3 0 1.650E-4
66 3.437E-2 8.256E-2 7.280E-1 8.104E-3 1.463E-2 1.309E-1 1.321E-3 0 1.624E-4
67 3.474E-2 8.259E-2 7.277E-1 8.214E-3 1.466E-2 1.306E-1 1.328E-3 0 1.602E-4
68 3.510E-2 8.238E-2 7.270E-1 8.319E-3 1.464E-2 1.311E-1 1.331E-3 0 1.576E-4
69 3.546E-2 8.250E-2 7.261E-1 8.425E-3 1.469E-2 1.313E-1 1.339E-3 0 1.554E-4
70 3.591E-2 8.226E-2 7.256E-1 8.530E-3 1.469E-2 1.315E-1 1.344E-3 0 1.528E-4
71 3.625E-2 8.222E-2 7.240E-1 8.659E-3 1.480E-2 1.325E-1 1.404E-3 0 1.737E-4
72 3.674E-2 8.201E-2 7.225E-1 8.789E-3 1.490E-2 1.334E-1 1.467E-3 0 1.851E-4
73 3.698E-2 8.156E-2 7.185E-1 8.903E-3 1.497E-2 1.341E-1 1.528E-3 3.231E-3 1.920E-4
74 3.740E-2 8.134E-2 7.155E-1 9.043E-3 1.506E-2 1.351E-1 1.594E-3 4.798E-3 1.971E-4
75 3.776E-2 8.098E-2 7.126E-1 9.163E-3 1.514E-2 1.359E-1 1.657E-3 6.525E-3 2.006E-4
76 3.810E-2 8.073E-2 7.095E-1 9.308E-3 1.522E-2 1.368E-1 1.732E-3 8.427E-3 2.038E-4
77 3.850E-2 8.026E-2 7.058E-1 9.422E-3 1.526E-2 1.373E-1 1.794E-3 1.161E-2 0
78 3.889E-2 7.995E-2 7.032E-1 9.569E-3 1.531E-2 1.379E-1 1.861E-3 1.327E-2 9.227E-5
79 3.933E-2 7.962E-2 6.999E-1 9.717E-3 1.537E-2 1.385E-1 1.924E-3 1.551E-2 9.384E-5
80 3.973E-2 7.937E-2 6.972E-1 9.873E-3 1.542E-2 1.391E-1 1.998E-3 1.712E-2 2.191E-4
81 4.017E-2 7.900E-2 6.945E-1 1.003E-2 1.547E-2 1.397E-1 2.072E-3 1.882E-2 2.725E-4
82 4.068E-2 7.870E-2 6.918E-1 1.018E-2 1.551E-2 1.402E-1 2.151E-3 2.041E-2 3.180E-4
83 4.112E-2 7.852E-2 6.891E-1 1.034E-2 1.556E-2 1.409E-1 2.236E-3 2.191E-2 3.547E-4
84 4.166E-2 7.826E-2 6.867E-1 1.051E-2 1.561E-2 1.413E-1 2.318E-3 2.325E-2 3.890E-4
85 4.216E-2 7.789E-2 6.840E-1 1.068E-2 1.566E-2 1.422E-1 2.409E-3 2.457E-2 4.208E-4
86 4.269E-2 7.765E-2 6.818E-1 1.084E-2 1.570E-2 1.426E-1 2.495E-3 2.582E-2 4.512E-4
87 4.325E-2 7.742E-2 6.791E-1 1.101E-2 1.577E-2 1.433E-1 2.582E-3 2.706E-2 4.937E-4
88 4.373E-2 7.716E-2 6.765E-1 1.121E-2 1.581E-2 1.441E-1 2.667E-3 2.827E-2 5.364E-4
89 4.435E-2 7.685E-2 6.742E-1 1.137E-2 1.585E-2 1.446E-1 2.754E-3 2.945E-2 5.760E-4
90 4.491E-2 7.659E-2 6.719E-1 1.155E-2 1.589E-2 1.451E-1 2.836E-3 3.056E-2 6.150E-4
91 4.552E-2 7.641E-2 6.700E-1 1.173E-2 1.596E-2 1.459E-1 2.904E-3 3.101E-2 6.139E-4
92 4.617E-2 7.616E-2 6.677E-1 1.191E-2 1.600E-2 1.467E-1 2.971E-3 3.176E-2 6.348E-4
93 4.682E-2 7.596E-2 6.659E-1 1.212E-2 1.605E-2 1.470E-1 3.058E-3 3.244E-2 6.588E-4
94 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
95 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
96 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
97 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
98 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
99 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
100 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
101 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
102 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
103 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
104 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
105 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
106 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
107 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
108 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
109 4.747E-2 7.578E-2 6.642E-1 1.230E-2 1.609E-2 1.476E-1 3.141E-3 3.281E-2 6.679E-4
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