Table F.2.
Transition probabilities (Aul) and effective collision strengths (Υlu) among the lowest ten levels of Ni III. See Table F.1 for level designations.
l | u | Aul | Temperature (1000 K) | ||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
(s−1) | 1.0 | 1.5 | 1.8 | 2.0 | 2.5 | 5.0 | 7.5 | 10.0 | 15.0 | 18.0 | 20.0 | 30.0 | 40.0 | ||
1 | 2 | 6.54(−2) | 3.380 | 3.300 | 3.210 | 3.150 | 2.980 | 2.490 | 2.330 | 2.260 | 2.180 | 2.140 | 2.120 | 2.010 | 1.900 |
1 | 3 | 4.45(−9) | 1.320 | 1.160 | 1.090 | 1.050 | 0.962 | 0.771 | 0.708 | 0.680 | 0.653 | 0.640 | 0.630 | 0.587 | 0.560 |
1 | 4 | 5.56(−3) | 1.580 | 1.420 | 1.360 | 1.320 | 1.240 | 1.050 | 0.954 | 0.900 | 0.855 | 0.840 | 0.830 | 0.805 | 0.780 |
1 | 5 | 5.85(−2) | 1.520 | 1.500 | 1.490 | 1.480 | 1.460 | 1.320 | 1.220 | 1.150 | 1.080 | 1.050 | 1.040 | 0.977 | 0.921 |
1 | 6 | 5.10(−15) | 0.330 | 0.355 | 0.365 | 0.370 | 0.370 | 0.370 | 0.363 | 0.360 | 0.360 | 0.360 | 0.360 | 0.360 | 0.350 |
1 | 7 | 1.07(−17) | 0.060 | 0.070 | 0.070 | 0.070 | 0.080 | 0.090 | 0.090 | 0.100 | 0.100 | 0.100 | 0.100 | 0.100 | 0.100 |
1 | 8 | 3.59(−1) | 0.490 | 0.500 | 0.505 | 0.510 | 0.530 | 0.620 | 0.696 | 0.770 | 0.882 | 0.926 | 0.950 | 1.020 | 1.020 |
1 | 9 | < 10(−10) | 0.062 | 0.061 | 0.060 | 0.060 | 0.059 | 0.056 | 0.054 | 0.053 | 0.052 | 0.052 | 0.052 | 0.055 | 0.062 |
1 | 10 | 1.22(−1) | 1.950 | 1.880 | 1.850 | 1.830 | 1.810 | 1.780 | 1.760 | 1.710 | 1.600 | 1.540 | 1.500 | 1.340 | 1.220 |
2 | 3 | 2.68(−2) | 1.900 | 1.900 | 1.880 | 1.870 | 1.820 | 1.670 | 1.630 | 1.600 | 1.580 | 1.550 | 1.540 | 1.460 | 1.390 |
2 | 4 | 4.95(−1) | 1.090 | 1.050 | 1.020 | 1.000 | 0.961 | 0.811 | 0.731 | 0.690 | 0.653 | 0.645 | 0.640 | 0.622 | 0.600 |
2 | 5 | 1.23(−1) | 0.750 | 0.777 | 0.790 | 0.800 | 0.810 | 0.790 | 0.755 | 0.730 | 0.713 | 0.705 | 0.700 | 0.675 | 0.640 |
2 | 6 | 4.46(−2) | 0.530 | 0.590 | 0.616 | 0.630 | 0.650 | 0.670 | 0.645 | 0.630 | 0.595 | 0.585 | 0.580 | 0.545 | 0.520 |
2 | 7 | 6.69(−15) | 0.110 | 0.120 | 0.125 | 0.130 | 0.140 | 0.140 | 0.133 | 0.130 | 0.130 | 0.130 | 0.130 | 0.120 | 0.120 |
2 | 8 | 1.83(−1) | 0.430 | 0.437 | 0.440 | 0.440 | 0.450 | 0.510 | 0.579 | 0.640 | 0.737 | 0.776 | 0.800 | 0.855 | 0.860 |
2 | 9 | < 10(−10) | 0.137 | 0.131 | 0.128 | 0.126 | 0.123 | 0.183 | 0.329 | 0.458 | 0.599 | 0.631 | 0.639 | 0.614 | 0.557 |
2 | 10 | 9.49(−3) | 0.012 | 0.011 | 0.010 | 0.010 | 0.009 | 0.007 | 0.008 | 0.009 | 0.009 | 0.009 | 0.009 | 0.009 | 0.008 |
3 | 4 | 2.16(−1) | 0.730 | 0.747 | 0.745 | 0.740 | 0.720 | 0.610 | 0.541 | 0.510 | 0.483 | 0.480 | 0.480 | 0.472 | 0.460 |
3 | 5 | 2.50(−2) | 0.460 | 0.460 | 0.460 | 0.460 | 0.460 | 0.450 | 0.443 | 0.440 | 0.440 | 0.445 | 0.450 | 0.442 | 0.430 |
3 | 6 | 1.88(−2) | 0.370 | 0.412 | 0.430 | 0.440 | 0.460 | 0.480 | 0.463 | 0.450 | 0.433 | 0.425 | 0.420 | 0.395 | 0.380 |
3 | 7 | 5.46(−2) | 0.180 | 0.205 | 0.220 | 0.230 | 0.240 | 0.250 | 0.250 | 0.240 | 0.230 | 0.225 | 0.220 | 0.210 | 0.200 |
3 | 8 | 4.62(−4) | 0.340 | 0.340 | 0.340 | 0.340 | 0.340 | 0.380 | 0.432 | 0.470 | 0.540 | 0.566 | 0.580 | 0.625 | 0.620 |
3 | 9 | 1.59(−1) | 0.025 | 0.025 | 0.024 | 0.024 | 0.023 | 0.020 | 0.018 | 0.017 | 0.015 | 0.015 | 0.014 | 0.013 | 0.012 |
3 | 10 | < 10(−10) | 0.007 | 0.006 | 0.006 | 0.006 | 0.006 | 0.005 | 0.005 | 0.005 | 0.004 | 0.004 | 0.004 | 0.004 | 0.004 |
4 | 5 | 1.02(−1) | 0.610 | 0.593 | 0.585 | 0.580 | 0.570 | 0.540 | 0.530 | 0.550 | 0.585 | 0.606 | 0.620 | 0.648 | 0.640 |
4 | 6 | 9.43(−2) | 0.360 | 0.343 | 0.335 | 0.330 | 0.320 | 0.300 | 0.297 | 0.300 | 0.317 | 0.325 | 0.330 | 0.340 | 0.330 |
4 | 7 | 2.87(−6) | 0.150 | 0.123 | 0.115 | 0.110 | 0.110 | 0.090 | 0.090 | 0.090 | 0.100 | 0.100 | 0.100 | 0.110 | 0.110 |
4 | 8 | 7.22(−4) | 0.390 | 0.390 | 0.395 | 0.400 | 0.410 | 0.490 | 0.559 | 0.620 | 0.697 | 0.731 | 0.750 | 0.788 | 0.790 |
4 | 9 | 1.27(+1) | 0.105 | 0.100 | 0.098 | 0.097 | 0.094 | 0.083 | 0.077 | 0.073 | 0.068 | 0.067 | 0.066 | 0.062 | 0.059 |
4 | 10 | < 10(−10) | 0.219 | 0.212 | 0.206 | 0.203 | 0.195 | 0.170 | 0.157 | 0.150 | 0.145 | 0.144 | 0.144 | 0.146 | 0.145 |
5 | 6 | 5.93(−4) | 0.480 | 0.522 | 0.540 | 0.550 | 0.570 | 0.570 | 0.570 | 0.570 | 0.580 | 0.585 | 0.590 | 0.590 | 0.580 |
5 | 7 | 3.07(−9) | 0.120 | 0.127 | 0.130 | 0.130 | 0.140 | 0.150 | 0.150 | 0.160 | 0.160 | 0.160 | 0.160 | 0.170 | 0.160 |
5 | 8 | 3.18(−5) | 0.330 | 0.330 | 0.330 | 0.330 | 0.330 | 0.400 | 0.462 | 0.500 | 0.535 | 0.550 | 0.560 | 0.578 | 0.570 |
5 | 9 | 9.85(−1) | 0.097 | 0.156 | 0.175 | 0.183 | 0.192 | 0.168 | 0.136 | 0.113 | 0.085 | 0.074 | 0.069 | 0.050 | 0.041 |
5 | 10 | < 10(−10) | 0.060 | 0.065 | 0.065 | 0.064 | 0.062 | 0.052 | 0.046 | 0.043 | 0.039 | 0.038 | 0.037 | 0.035 | 0.034 |
6 | 7 | 8.71(−4) | 0.300 | 0.300 | 0.295 | 0.290 | 0.290 | 0.260 | 0.243 | 0.230 | 0.230 | 0.225 | 0.220 | 0.212 | 0.210 |
6 | 8 | 1.59(−21) | 0.190 | 0.190 | 0.190 | 0.190 | 0.190 | 0.230 | 0.257 | 0.270 | 0.287 | 0.295 | 0.300 | 0.300 | 0.300 |
6 | 9 | 5.96(+0) | 0.135 | 0.137 | 0.140 | 0.141 | 0.148 | 0.213 | 0.292 | 0.358 | 0.442 | 0.473 | 0.488 | 0.527 | 0.534 |
6 | 10 | < 10(−10) | 0.036 | 0.037 | 0.038 | 0.038 | 0.041 | 0.067 | 0.100 | 0.128 | 0.166 | 0.180 | 0.187 | 0.204 | 0.206 |
7 | 8 | 2.50(−25) | 0.070 | 0.070 | 0.070 | 0.070 | 0.070 | 0.080 | 0.087 | 0.090 | 0.100 | 0.100 | 0.100 | 0.100 | 0.100 |
7 | 9 | < 10(−10) | 0.065 | 0.065 | 0.067 | 0.069 | 0.082 | 0.244 | 0.386 | 0.459 | 0.491 | 0.481 | 0.471 | 0.405 | 0.348 |
7 | 10 | < 10(−10) | 0.053 | 0.051 | 0.049 | 0.048 | 0.047 | 0.051 | 0.059 | 0.062 | 0.062 | 0.060 | 0.058 | 0.051 | 0.045 |
8 | 9 | < 10(−10) | 0.249 | 0.242 | 0.238 | 0.236 | 0.232 | 0.221 | 0.217 | 0.214 | 0.211 | 0.209 | 0.208 | 0.204 | 0.201 |
8 | 10 | 2.97(−6) | 0.361 | 0.320 | 0.300 | 0.290 | 0.268 | 0.216 | 0.194 | 0.179 | 0.159 | 0.151 | 0.147 | 0.132 | 0.121 |
9 | 10 | < 10(−10) | 0.173 | 0.167 | 0.163 | 0.160 | 0.155 | 0.142 | 0.142 | 0.146 | 0.150 | 0.151 | 0.150 | 0.144 | 0.137 |
Notes: Numbers in parentheses correspond to powers of ten. Entries for transitions among the lowest eight levels for temperatures ≤40000 K were computed following the methods outlined in Storey et al. (2016). All other entries are based on Ramsbottom et al. (2007); in this latter approach, transition probabilities Aul < 10−10 s−1 are deemed too small to be significant and we report these as upper limits. A complete set of transition probabilities and effective collision strengths among the lowest 43 levels of Ni III and extending to 105 K is available in electronic format at the CDS.
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