Contents

• Energy levels and transition probabilities for boron-like Fe XXII
• 1 Introduction
• 2 Method of calculation
• 3 Results and discussion
• 4 Conclusions
• References
• 5 Online Material

A&A 455, 1157-1160 (2006)
DOI: 10.1051/0004-6361:20064822

Energy levels and transition probabilities for boron-like Fe XXII^,

V. Jonauskas^1,2 - P. Bogdanovich² - F. P. Keenan¹ - R. Kisielius^1,2 - M. E. Foord³ - R. F. Heeter³ - S. J. Rose⁴ - G. J. Ferland⁵ - P. H. Norrington⁶

1 - Department of Physics and Astronomy, The Queen's University of Belfast, Belfast BT7 1NN, Northern Ireland, UK
2 - Institute of Theoretical Physics and Astronomy of Vilnius University, A. Gostauto 12, 01108 Vilnius, Lithuania
3 - University of California, Lawrence Livermore National Laboratory, Livermore, CA 94551, USA
4 - Department of Physics, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UK
5 - Department of Physics, University of Kentucky, Lexington, KY 40506, USA
6 - Department of Applied Mathematics and Theoretical Physics, The Queen's University of Belfast, Belfast BT7 1NN, Northern Ireland, UK

Received 6 January 2006 / Accepted 17 May 2006

Abstract
The Multiconfiguration Dirac-Fock method is used to calculate the energies of the 407 lowest levels in Fe XXII. These results are cross-checked using a suite of codes which employ the configuration interaction method on the basis set of transformed radial orbitals with variable parameters, and takes into account relativistic corrections in the Breit-Pauli approximation. Transition probabilities, oscillator and line strengths are presented for electric dipole (E1), electric quadrupole (E2) and magnetic dipole (M1) transitions among these levels. The total radiative transition probabilities, as well as the five largest values from each level be it of E1, M1, E2, M2, or E3 type, are also provided. Finally, the results are compared with data compiled by NIST.

Key words: atomic data

1 Introduction

Physical processes and conditions in astrophysical sources can be understood through the use of theoretical models to analyse high resolution spectral observations. In particular, X-ray spectra from iron L-shell ions are prominent candidates for astrophysics plasma diagnostics, as their emission lines are observed in the wavelength range from 6-18 Å, covered with large effective areas by X-ray telescopes on board the space observatories Chandra and XMM-Newton. Behar et al. (2001) identified Fe XXII lines in a spectrum of the Capella binary system obtained by the High Energy Transmission Grating Spectrometer on board Chandra, while Kinkhabwala et al. (2002) observed Fe XXII in the Seyfert 2 galaxy NGC 1068. To reliably analyse such spectra requires an accurate knowledge of wavelengths and radiative transition rates, obtained from calculations or experiment.

Numerous observations of boron-like iron have been previously reported in the X-ray spectra of the Sun (McKenzie et al. 1985; Phillips et al. 1996; Fawcett et al. 1987; Doschek et al. 1981,1973; Phillips et al. 1982). Wargelin et al. (1998) have presented an analysis of the density sensitivity of Fe XXII L-shell lines in plasma obtained in the Princeton Large Torus tokamak. They analysed the intensity ratios of 4d_5/2 - 2p_3/2 and 4d_3/2 - 2p_1/2 lines using the HULLAC atomic physics package (Bar-Shalom et al. 2001). Recently, Chen et al. (2004) used a radiative-collisional model to predict the density of a plasma produced using the Electron Beam Ion Trap at Lawrence Livermore National Laboratory. They showed that the line ratios of the 2p-3d transitions in boron-like iron are sensitive to the electron density in the range $n_{\rm e} = 10^{13}{-}10^{15}$ cm^-3. Earlier, electron-excitation rate calculations for 45 fine-structure levels, using the Breit-Pauli formulation of the R-matrix method, were performed by Zhang & Pradhan (1997). Badnell et al. (2001) used the AUTOSTRUCTURE code (Badnell 1997,1986) to generate radial orbitals and atomic structure for 204-level close-coupling calculations in Fe XXII. A large set of energy levels is presented in the CHIANTI database at http://wwwsolar.nrl.navy.mil/chianti.html.

The aim of the present paper is extend our series of calculations for iron ions (Jonauskas et al. 2004a,b,2005), by providing highly reliable energy levels and radiative transition rates for Fe XXII up to the n=5 complex. We note that in photoionized plasmas these high-lying levels will not in general be populated via electron impact (although collisional redistribution among the levels may play a role), but rather by a range of processes including recombination and charge transfer (Savin 2001). Transitions in Fe XXII from high-lying levels having 5d electrons were observed by Fawcett et al. (1987) in a solar flare spectrum. Wargelin et al. (1998) identified transitions from 2s²4d¹, 2s¹2p¹4p¹, 2s¹2p¹5p¹, 2s²5d¹, 2s¹2p¹5d¹ and 2s²6d¹ configurations which are populated in a radiative-collisional model by electron collisions from metastable state.

In the present paper calculations are performed using the multiconfiguration Dirac-Fock (MCDF) approach. Energies of the lowest 407 levels, plus E1, E2 and M1 type radiative transition probabilities, as well as line and oscillator strengths among the levels of Fe XXII, are provided. The calculated results are compared with data compiled by NIST, as well as results obtained from other codes. The agreement between the length and velocity forms of electric transition operators is checked for the strongest transitions as an additional measure of the accuracy for the data obtained. The total radiative probabilities and five strongest probabilities required for calculating branching ratios of levels are presented as well.

2 Method of calculation

Results were obtained using the multiconfiguration Dirac-Fock (MCDF) method employed in the GRASP code of Grant et al. (1980) and Parpia et al. (1996) (http://www.am.qub.ac.uk/DARC). To cross-check our MCDF data, we used a code developed by Bogdanovich & Karpuskiene (1999), which adopts the configuration interaction (CI) method on the basis of transformed radial orbitals (TROs) with variable parameters, including relativistic effects in the Breit-Pauli approximation ( CITRO).

2.1 MCDF approach

In the MCDF approach, intermediate coupling wavefunctions $\Psi_{\gamma} (J)$ are constructed by using an expansion of the form:

$$% \Psi_{\gamma} (J)=\sum\limits_{\alpha}c_{\gamma}(\alpha J)~\Phi (\alpha J),$$ (1)

where configuration state functions (CSFs) $\Phi (\alpha J)$ are expressed as antisymmetrized products of two-component orbitals

$$% \phi (r)=\frac{1}{r}\left( \begin{array}{rc} P_{nlj}(r) & ... ...bar{l}j}(r) & \chi _{\bar{l}jm}(\hat{r}) \end{array}\right).$$ (2)

Here P_nlj(r) and $Q_{n\bar{l}j}(r)$ are the large and small radial components of one-electron wavefunctions and  $\chi _{ljm}(\hat{r})$ are the two component Pauli spherical spinors. Two-component orbitals are obtained as the self-consistent solutions of the Dirac-Fock equations systematically increasing CI basis. Direct and indirect relativistic effects, when the contraction of inner orbitals leads to more effective screening of the nucleus for valence orbitals, are included in the relativistic wavefunctions by solving MCDF equations.

The configuration mixing coefficients $c_{\gamma}$ are obtained through diagonalization of the Dirac-Coulomb-Breit Hamiltonian:

$$% H^{{\rm DF}} = \sum\limits_{i}\ h_{i}^{\rm D} + \sum\limit... ...}\ h_{ij}^{{\rm e}} + \sum\limits_{i<j}\ h_{ij}^{{\rm trans}},$$ (3)

where $h_{i}^{{\rm D}}$ is one-electron Dirac Hamiltonian, $h_{ij}^{{\rm e}}$ is the instantaneous Coulomb repulsion. The effects of the transverse interaction  $h_{ij}^{{\rm trans}}$ that corresponds to the Breit interaction:

$$% h_{ij}^{{\rm Breit}}=-\frac{\alpha _{i}\cdot \alpha _{j}}{2... ...alpha _{i}\cdot r_{ij})(\alpha _{j}\cdot r_{ij})}{2r_{ij}^{3}}$$ (4)

in the low-frequency limit were evaluated in the first order of perturbation expansion. QED corrections, which include vacuum polarization and self-energy (known as the Lamb shift), are considered in the first order of perturbation theory.

One-electron excitations from the 2s and 2p orbitals of the 1s²2s²2p¹, 1s²2s¹2p² and 1s²2p³ configurations up to the 8k orbital, as well as two- and three-electron excitations from orbitals with n=2 to all possible combinations of two or three electrons in the shells up to n=3, were employed to generate one-electron wavefunctions as a basis set for CSFs in the MCDF method. Additionally, to extend the CI basis and obtain higher accuracy, an additional 14 configurations with electrons in n=4 are included, namely: 1s²2s¹4s², 1s²2s¹4p², 1s²2s¹4d², 1s²2s¹4f², 1s²2p¹4s², 1s²2p¹4p², 1s²2p¹4d², 1s²2p¹4f², 1s²2s¹3p¹4p¹, 1s²2s¹3p¹4f¹, 1s²3s¹3p¹4p¹, 1s²3s¹3p¹4f¹, 1s²2p¹3p¹4s¹, 1s²2p¹3p¹4d¹. The total number of CSFs in our MCDF calculations is 2253.

2.2 CITRO method

In the nonrelativistic, multiconfiguration Hartree-Fock approach, intermediate coupling wavefunctions  $\Psi_{\gamma} (J)$ being eigenfunctions of Coulomb-Breit-Pauli Hamiltonian are expanded in terms of CSFs $\Phi (\alpha LSJ)$ obtained in the LSJ-coupling scheme:

$$% \Psi_{\gamma} (J)=\sum\limits_{\alpha LS}c_{\gamma}(\alpha LSJ)~\Phi (\alpha LSJ)$$ (5)

CSFs are formed from a basis of one-electron spin orbitals:

$$% \phi (r)=\frac{1}{r}P_{nl}(r)Y_{lm_{l}}(\vartheta ,\phi )\chi _{m_{s}}.$$ (6)

The number of CSFs in the intermediate coupling wavefunction expansion (5) is limited. Hence transformed radial orbitals with variable parameters were proposed by Bogdanovich & Karpuskiene (1999) to mimic the correlation effects from omitted CSFs:

$$% P_{nl}^{{\rm T}}(r)=N\left\{ f(r)P_{nl}(r)-\sum_{n^{\prime ... ...<n}c_{n^{\prime \prime },n}P_{n^{\prime \prime }l}(r)\right\}.$$ (7)

Here N is a normalization factor, $c_{n^{\prime \prime },n}$ denotes the corresponding overlap integral, and f(r) is a transforming function:

$$% f(r)=r^{k}\exp (-Ar^{m})$$ (8)

with variable parameters k, m and A ($k \ge 0$, $k \ge l - l'$, m > 0, A > 0). The variation of all parameters ensure the largest corrections of correlation energies obtained in the second order of perturbation theory using admixed configurations with excited electrons. A Schmidt orthogonalization procedure is employed for TROs in (7).

The Coulomb-Breit-Pauli Hamiltonian is used for our configuration interaction calculations which lead to the expansion coefficients  $c_{\gamma}(\alpha LSJ)$ and the corresponding energies for levels. This Hamiltonian includes spin-orbit  $h_{i}^{{\rm so}}$, spin-other-orbit $h_{ij}^{{\rm soo}}$ and spin-spin $h_{ij}^{{\rm ss}}$ corrections as well as orbit-orbit corrections  $h_{ij}^{{\rm oo}}$ within a shell of equivalent electrons:

$$% H^{{\rm BP}} \sum\limits_{i}\ \left(-\frac{1}{2} \nabla^2_{i} - Z/r_{i}\right) + \sum\limits_{i<j}\ \frac{1}{r_{ij}} + \sum\limits_{i}\ h_{i}^{{\rm so}}$$ =

$$+ \sum\limits_{i<j}\ h_{ij}^{{\rm soo}} + \sum\limits_{i<j}\ h_{ij}^{{\rm ss}} + \sum\limits_{i<j}\ h_{ij}^{{\rm oo}},$$ (9)

where $H^{{\rm BP}}$ is expressed in atomic units. Orbit-orbit interactions between shells omitted in our CITRO calculations are usually smaller than within shells.

The frozen core approximation is used to obtain Hartree-Fock radial orbitals with $n \le 7$. To include correlation effects from higher CSFs, the obtained basis is supplemented by TROs with principal quantum numbers $8 \le n \le 10$ and orbital quantum numbers $l \le 7$. The large number of admixed configurations is reduced, leaving only configurations with significant influence on the energies of the adjusted configurations. For this, the method presented by Bogdanovich et al. (2002) and Bogdanovich & Momkauskaite (2004) is adopted. The total number of CSFs with odd parity is 2115, and the number with even parity is 1987 in our CITRO calculations.

3 Results and discussion

In Table 1 we list energies of the 407 lowest levels of Fe XXII obtained with the GRASP code. These levels correspond to 1s²2s²2p¹, 1s²2s¹2p², 1s²2p³, 1s²2s²3l, 1s²2s¹2p¹3l, 1s²2p²3l, 1s²2s²4l', 1s²2s¹2p¹4l', 1s²2p²4l', 1s²2s²5l'', 1s²2s¹2p¹5l'', 1s²2s²6l''' (l = 0,1,2, l' = 0,1,2,3, l'' = 0,1,2,3,4 and l''' = 0,1,2,3,4,5) configurations. Energy levels are given in cm^-1 relative to the ground state 1s²2s²2p^{1 2}P_0.5, along with the leading percentage compositions  $c_{\gamma}(\alpha J)^2$ (where these exceed 10%) from the expansion relation Eq. (1) for intermediate coupling wavefunctions. The expansion coefficients for the intermediate coupling wavefunctions with CSFs presented in the LSJ-coupling scheme (5) are obtained from the expansion terms of intermediate coupling wavefunctions with CSFs presented in jj-coupling scheme (1). Diagonalization of Dirac-Coulomb-Breit matrix gives the expansion coefficients for intermediate coupling wavefunctions with CSFs constructed from two-component orbitals. The indices for the levels provided in the first column of Table 1 are used in all subsequent tables.

Some excited levels due to strong intermediate coupling are assigned to the same CSFs. In Table 2 new LSJ-coupling spectroscopic notations are proposed for the levels which have the same CSFs with primary contributions to the intermediate coupling wavefunctions. For this, the technique presented in our earlier paper for Fe XIX (Jonauskas et al. 2004b) is used.

In Table 3 we compare our calculated energy levels with values compiled by NIST (National Institute for Standards and Technology: www.physics.nist.gov) whose data are commonly used as a reference set. Fairly good agreement is obtained for the MCDF calculations, with the many energy levels agreeing to better than within 1% with the NIST recommended values. However, some excited energy levels (indices 29, 55, 59, 69, 74, 174 and 195) differ by up to 2% from NIST data. As well, our absolute values of energies for two levels (55 and 174) show the largest deviations from the NIST recommended values, while another five levels (29, 59, 69, 74 and 195) have MCDF absolute energies lower than those from NIST. To cross-check our results for these levels, we present data from CITRO calculations. For both our calculations, the highly excited levels show the similar discrepancies from NIST values. On the other hand, the MCDF energies of levels 174 (1s²2s¹2p¹ (³P) 4d^{1 2}F_3.5) and 195 (1s²2s¹2p¹ (¹P) 4d^{1 2}F_3.5) show good agreement with NIST data after their values are interchanged. This suggests that there are some typographical errors in the NIST data for these levels. The calculated energies of level 29 (1s² 2s¹ 2p¹(³P)3p^{1 2}P_0.5) has similar discrepancies ($\sim$$1.5\%$) for both calculations presented in Table 3, but our MCDF result is closer to the NIST recommended value. As well, our CITRO and MCDF calculations show the same percentage composition for the intermediate coupling wavefunction of the level. The energy of the 1s² 2s¹ 2p¹ (³P) 3p^1 2P_0.5 level (29) is lower than that of 1s² 2s¹ 2p¹ (³P) 3p^1 2P_1.5 (28) in the NIST data, while the ordering of both levels in our calculations is opposite to the NIST order. It suggests that a bigger CI basis may be required for the MCDF calculations to obtain better agreement with the NIST values for the level. However, the energy for the level obtained by Zhang & Pradhan (1997) with SUPERSTRUCTURE (Eissner et al. 1974), and the value provided by Badnell et al. (2001) from their AUTOSTRUCTURE (Badnell 1997,1986) calculations show similar differences from NIST, and the same order as in our data.

For another five levels (55, 59, 69 and 74) with the largest discrepancies from NIST values, our MCDF and CITRO energies are in close agreement with the AUTOSTRUCTURE values of Badnell et al. (2001) and, in general, are slightly closer to the NIST data. Furthermore, as will be seen later, some transitions from those levels have largest discrepancies for line strengths compared with the NIST values. Additionally, our calculated lifetimes for the levels are presented in Table 3, to have an additional way to estimate the accuracy of our calculations. Differences between the calculated lifetimes for those levels is less than 10%, which confirm the accuracy of our results.

Energy levels and intermediate coupling wavefunctions calculated with the configuration interaction method have been employed to compute matrix elements of transition operators, which subsequently are adopted for the calculation of transition probabilities, line and oscillator strengths. The wavelengths and line strengths are presented in Table 4, where our transition data are compared with NIST results. All line strengths belong to E1 type transitions except one from the first excited level which corresponds to M1 type transition. E2 type transition from the level is much weaker (MCDF and NIST line strengths equal to 2.10 $\times$ 10^-3 and 2.15 $\times$ 10^-3 correspondingly). The length form is used for electric transitions, as they are less sensitive to the accuracy of wavefunction compared with results obtained in the velocity form of the transition operator. The wavelengths for many transitions agree to better than within 1% with the NIST data. The largest differences for the wavelengths are obtained for transitions between energy levels which showed largest discrepancies from NIST energies. The largest discrepancy for line strengths is observed for the weak transition (f = 3 $\times$ 10^-5) from the 2s¹2p^2 2P_0.5 level (8) to 2s²2p^1 2P_1.5 (2). The length and velocity forms differ by a factor of 3.5, while our calculated MCDF and CITRO line strengths coincide within 20% for the transition. Furthermore, the contribution of the transition to the lifetime of the level is very small. The line strengths for the transitions from 2s²4s^1 2S_0.5 (126) to the first and second levels of the ground configuration differ by 80% and 29%, respectively, from the NIST values, but are in the limits of uncertainties provided by NIST.

Additionally, large discrepancies are observed for some transitions from the above mentioned levels which showed the largest deviations for energy levels compared with the NIST values. The line strengths for transitions $55 \rightarrow 9$, $55 \rightarrow 10$, $59 \rightarrow 8$, $69 \rightarrow 8$, $74 \rightarrow 8$, $174 \rightarrow 7$ and $195 \rightarrow 7$ differ by 29% to up to a factor of 4. The contributions to the lifetimes of those dipole allowed transitions vary from 7% ( $74 \rightarrow 8$) to 84% ( $195 \rightarrow 7$) (Table 5). The large discrepancies observed for transitions from levels 174 and 195 can be explained by a typographical error in the NIST data. As in a case of energy levels, our line strengths and wavelengths for those transitions are in good agreement with the NIST line strengths, after the NIST values are interchanged. Finally, our MCDF results for all those transitions with large discrepancies with NIST line strengths are in close agreement with the CITRO ones. It is possible that the determination of all those energy levels is uncertain in the NIST database. Additionally, the fairly good agreement between length and velocity forms for all those transitions indicate that our transition characteristics are quite accurate and reliable.

Transition probabilities, line and oscillator strengths are calculated for radiative E1, E2, E3, M1 and M2 type transitions among the presented 407 energy levels of Fe XXII. We provide the transition wavelengths, probabilities, oscillator strengths and line strengths of E1, E2 and M1 type for Fe XXII in Tables 6-8. Only the strongest transitions are presented here for every type of transition: electric dipole transitions with $f \ge 0.001$, electric quadrupole with $f \ge 10^{-8}$ and magnetic dipole with $f \ge 10^{-8}$. The relation between length (Babushkin gauge in the relativistic approach) and velocity (Coulomb gauge) forms are provided for both electric transitions to have an additional indicator of accuracy of our MCDF results. The difference between both forms for many strong E1 type transitions ($f \ge 0.1$) does not exceed 20%. Only 4 transitions from highly excited levels have differences larger than 20% but less than 40%. On the other hand, the contribution of these transitions to the lifetimes of the levels is much smaller than 1%. Finally, the length and velocity forms of the strongest electric dipole transitions ($f \ge 0.1$) agree to better than within 10%, with an average deviation of only 1.8% for 457 transitions. For many E2 transitions, the two forms agree to better than within 10%.

In Table 5 we provide the five largest spontaneous radiative transition probabilities from each level, and the sum of all E1, E2, E3, M1 and M2 radiative transition probabilities from the corresponding level to all lower levels. The sums of radiative transition probabilities are important for branching ratios, while their inverse values are equal to the lifetimes of the levels. The contribution to the lifetimes of levels for many forbidden electric quadrupole and magnetic dipole transitions is negligible and does not exceed 1%. However, the highly excited 2s¹2p¹ (³P) 3p^1 4D_0.5 (33) and 2p² (¹D) 3d^1 2G_0.5 (114) levels decay primarily through E2 type transitions. For another two levels, i.e. 2p² (³P) 3d^1 4D_0.5 (97) and 2p² (³P) 3d^1 4F_0.5 (96), E2 type transitions contribute 48% and 46%, respectively. As well, the first excited level decays mainly due to magnetic dipole transition.

4 Conclusions

In this paper, energy levels, electric dipole, electric quadrupole and magnetic dipole radiative transition rates, oscillator and line strengths have been reported for the lowest 407 levels in Fe XXII in the MCDF approximation. The characteristics of the levels in the LSJ-coupling scheme have been provided and checked for their completeness. Calculated values have been compared with NIST recommended values. Breit-Pauli energy levels and electric dipole transition characteristics in the basis set of transformed radial orbitals with variable parameters were used to cross-check the accuracy of our results. Likely typographical errors for Fe XXII have been found in both the NIST energy levels and transition characteristics for the highly excited 2s¹2p¹ (³P) 4d^1 2F_3.5 and 2s¹2p¹ (¹P) 4d^1 2F_3.5 levels.

The forbidden transitions have been taken into account to obtain total radiative transition probabilities from levels. The total radiative probabilities allow estimates of the lifetimes of the presented states, and are also important for the calculation of branching ratios. It was found that the highly excited 2s¹2p¹ (³P) 3p^1 4D_0.5 and 2p² (¹D) 3d^1 2G_0.5 levels mainly decay due to forbidden E2 type transitions. Their contributions to the lifetimes of the 2p² (³P) 3d^1 4D_0.5 and 2p² (³P) 3d^1 4F_0.5 levels is 48% and 46%, respectively. The first excited level decays mainly through M1 type transition. For each level, the five strongest transition probabilities are presented.

To conclude, the comparison with the NIST recommended wavelengths and radiative transition data shows that all the presented theoretical results are reliable, and may be successfully used for the interpretation of astronomical and other spectral observations.

Acknowledgements

FPK and SJR are grateful to AWE Aldermaston for the award of William Penney Fellowships. This work was supported by PPARC and EPSRC, and also by NATO Collaborative Linkage Grant CLG.979443. We are also grateful to the Defence Science and Technology Laboratory (dstl) for support under the Joint Grants Scheme.

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5 Online Material

   

Table 1: MCDF results for energy levels of Fe XXII. The energies of levels are presented relative to the ground energy. The leading percentage compositions (>10%) of levels are provided in the last column.

Index	Configuration	LS	J	E (cm-1)	Composition
1	1s2 2s2 2p1	2P	0.5	${\boldmath -}$192757192	98%
2	1s2 2s2 2p1	2P	1.5	117953	97%
3	1s2 2s1 2p2	4P	0.5	402902	96%
4	1s2 2s1 2p2	4P	1.5	458031	99%
5	1s2 2s1 2p2	4P	2.5	511295	94%
6	1s2 2s1 2p2	2D	1.5	741538	95%
7	1s2 2s1 2p2	2D	2.5	763743	94%
8	1s2 2s1 2p2	2P	0.5	861921	60% + 37% 1s2 2s1 2p2 2S
9	1s2 2s1 2p2	2S	0.5	986277	59% + 39% 1s2 2s1 2p2 2P
10	1s2 2s1 2p2	2P	1.5	1000692	95%
11	1s2 2p3	4S	1.5	1260179	90%
12	1s2 2p3	2D	1.5	1405688	82% + 12% 1s2 2p3 2P
13	1s2 2p3	2D	2.5	1435674	100%
14	1s2 2p3	2P	0.5	1582452	98%
15	1s2 2p3	2P	1.5	1639226	78% + 16% 1s2 2p3 2D
16	1s2 2s2 3s1	2S	0.5	8111550	95%
17	1s2 2s2 3p1	2P	0.5	8292834	91%
18	1s2 2s2 3p1	2P	1.5	8326008	91%
19	1s2 2s1 2p1 (3P) 3s1	4P	0.5	8471848	96%
20	1s2 2s2 3d1	2D	1.5	8491152	95%
21	1s2 2s2 3d1	2D	2.5	8501013	95%
22	1s2 2s1 2p1 (3P) 3s1	4P	1.5	8502156	91%
23	1s2 2s1 2p1 (3P) 3s1	2P	0.5	8577184	92%
24	1s2 2s1 2p1 (3P) 3s1	4P	2.5	8584529	98%
25	1s2 2s1 2p1 (3P) 3p1	4D	0.5	8630313	76% + 21% 1s2 2s1 2p1 (3P) 3p1 2P
26	1s2 2s1 2p1 (3P) 3p1	4D	1.5	8657024	75% + 18% 1s2 2s1 2p1 (3P) 3p1 2P
27	1s2 2s1 2p1 (3P) 3s1	2P	1.5	8663895	90%
28	1s2 2s1 2p1 (3P) 3p1	2P	1.5	8695560	30% + 25% 1s2 2s1 2p1 (3P) 3p1 4S + 17% 1s2 2s1 2p1 (3P) 3p1 4P
29	1s2 2s1 2p1 (3P) 3p1	2P	0.5	8704356	66% + 22% 1s2 2s1 2p1 (3P) 3p1 4D
30	1s2 2s1 2p1 (3P) 3p1	4D	2.5	8707420	90%
31	1s2 2s1 2p1 (3P) 3p1	4P	0.5	8734123	90%
32	1s2 2s1 2p1 (3P) 3p1	2D	1.5	8748534	36% + 31% 1s2 2s1 2p1 (3P) 3p1 4S + 15% 1s2 2s1 2p1 (3P) 3p1 4P
33	1s2 2s1 2p1 (3P) 3p1	4D	3.5	8781923	99%
34	1s2 2s1 2p1 (3P) 3p1	4P	1.5	8791861	44% + 25% 1s2 2s1 2p1 (3P) 3p1 2D + 19% 1s2 2s1 2p1 (3P) 3p1 2P
35	1s2 2s1 2p1 (3P) 3d1	4F	1.5	8808079	89%
36	1s2 2s1 2p1 (3P) 3p1	4S	1.5	8809920	37% + 22% 1s2 2s1 2p1 (3P) 3p1 4P + 19% 1s2 2s1 2p1 (3P) 3p1 2D
37	1s2 2s1 2p1 (3P) 3p1	4P	2.5	8809932	68% + 23% 1s2 2s1 2p1 (3P) 3p1 2D
38	1s2 2s1 2p1 (3P) 3d1	4F	2.5	8827013	85% + 11% 1s2 2s1 2p1 (3P) 3d1 4D
39	1s2 2s1 2p1 (3P) 3p1	2D	2.5	8857624	73% + 24% 1s2 2s1 2p1 (3P) 3p1 4P
40	1s2 2s1 2p1 (3P) 3d1	4F	3.5	8857700	79% + 17% 1s2 2s1 2p1 (3P) 3d1 4D
41	1s2 2s1 2p1 (3P) 3d1	4P	2.5	8868503	46% + 23% 1s2 2s1 2p1 (3P) 3d1 4D + 23% 1s2 2s1 2p1 (3P) 3d1 2D
42	1s2 2s1 2p1 (3P) 3d1	4D	1.5	8878309	59% + 25% 1s2 2s1 2p1 (3P) 3d1 4P
43	1s2 2s1 2p1 (3P) 3d1	4D	0.5	8881447	84%
44	1s2 2s1 2p1 (3P) 3p1	2S	0.5	8888579	79%
45	1s2 2s1 2p1 (1P) 3s1	2P	0.5	8891445	91%
46	1s2 2s1 2p1 (1P) 3s1	2P	1.5	8892983	82%
47	1s2 2s1 2p1 (3P) 3d1	2D	1.5	8916505	67% + 11% 1s2 2s1 2p1 (3P) 3d1 2P
48	1s2 2s1 2p1 (3P) 3d1	4F	4.5	8925683	100%
49	1s2 2s1 2p1 (3P) 3d1	2D	2.5	8930222	43% + 28% 1s2 2s1 2p1 (3P) 3d1 2F + 13% 1s2 2s1 2p1 (3P) 3d1 4D
50	1s2 2s1 2p1 (3P) 3d1	4D	3.5	8955370	79% + 19% 1s2 2s1 2p1 (3P) 3d1 4F
51	1s2 2s1 2p1 (3P) 3d1	4D	2.5	8966348	50% + 35% 1s2 2s1 2p1 (3P) 3d1 4P
52	1s2 2s1 2p1 (3P) 3d1	4P	1.5	8972247	68% + 29% 1s2 2s1 2p1 (3P) 3d1 4D
53	1s2 2s1 2p1 (3P) 3d1	4P	0.5	8975643	91%
54	1s2 2s1 2p1 (3P) 3d1	2F	2.5	9004790	55% + 28% 1s2 2s1 2p1 (3P) 3d1 2D
55	1s2 2s1 2p1 (3P) 3d1	2P	1.5	9043521	78% + 10% 1s2 2s1 2p1 (3P) 3d1 2D
56	1s2 2s1 2p1 (3P) 3d1	2F	3.5	9060831	97%
57	1s2 2s1 2p1 (1P) 3p1	2P	0.5	9067791	79% + 10% 1s2 2p2 (3P) 3s1 2P
58	1s2 2s1 2p1 (1P) 3p1	2D	1.5	9074412	64% + 26% 1s2 2s1 2p1 (1P) 3p1 2P
59	1s2 2s1 2p1 (3P) 3d1	2P	0.5	9078984	94%
60	1s2 2s1 2p1 (1P) 3p1	2D	2.5	9093833	91%
61	1s2 2s1 2p1 (1P) 3p1	2P	1.5	9103377	59% + 25% 1s2 2s1 2p1 (1P) 3p1 2D
62	1s2 2p2 (3P) 3s1	4P	0.5	9121949	55% + 27% 1s2 2s1 2p1 (1P) 3p1 2S
63	1s2 2s1 2p1 (1P) 3p1	2S	0.5	9153543	54% + 33% 1s2 2p2 (3P) 3s1 4P
64	1s2 2p2 (3P) 3s1	4P	1.5	9193266	95%
65	1s2 2p2 (3P) 3s1	4P	2.5	9238570	80% + 16% 1s2 2p2 (1D) 3s1 2D
66	1s2 2s1 2p1 (1P) 3d1	2F	3.5	9250872	93%
67	1s2 2s1 2p1 (1P) 3d1	2F	2.5	9253139	85%
68	1s2 2p2 (3P) 3s1	2P	0.5	9262279	77%
69	1s2 2s1 2p1 (1P) 3d1	2D	1.5	9263777	93%
70	1s2 2p2 (3P) 3p1	4D	0.5	9265730	50% + 16% 1s2 2p2 (3P) 3p1 2S
71	1s2 2s1 2p1 (1P) 3d1	2D	2.5	9276912	90%
72	1s2 2p2 (3P) 3s1	2P	1.5	9298666	47% + 41% 1s2 2p2 (1D) 3s1 2D
73	1s2 2s1 2p1 (1P) 3d1	2P	0.5	9298930	89%
74	1s2 2s1 2p1 (1P) 3d1	2P	1.5	9300838	62% + 18% 1s2 2p2 (3P) 3p1 4D
75	1s2 2p2 (3P) 3p1	4D	1.5	9318728	53% + 32% 1s2 2s1 2p1 (1P) 3d1 2P
76	1s2 2p2 (3P) 3p1	2S	0.5	9326572	44% + 33% 1s2 2p2 (3P) 3p1 4D + 21% 1s2 2p2 (3P) 3p1 4P
77	1s2 2p2 (3P) 3p1	4P	1.5	9360271	32% + 25% 1s2 2p2 (3P) 3p1 2D + 20% 1s2 2p2 (3P) 3p1 4D
78	1s2 2p2 (3P) 3p1	4D	2.5	9369611	86%
79	1s2 2p2 (3P) 3p1	4P	0.5	9385693	64% + 21% 1s2 2p2 (3P) 3p1 2S
80	1s2 2p2 (1D) 3s1	2D	2.5	9386490	77% + 18% 1s2 2p2 (3P) 3s1 4P
81	1s2 2p2 (3P) 3p1	4P	2.5	9390309	43% + 23% 1s2 2p2 (3P) 3p1 2D + 20% 1s2 2p2 (1D) 3p1 2D
82	1s2 2p2 (3P) 3p1	2D	1.5	9405884	43% + 32% 1s2 2p2 (3P) 3p1 4P + 14% 1s2 2p2 (1D) 3p1 2D
83	1s2 2p2 (1D) 3s1	2D	1.5	9406759	53% + 37% 1s2 2p2 (3P) 3s1 2P
84	1s2 2p2 (3P) 3p1	4D	3.5	9414721	80% + 17% 1s2 2p2 (1D) 3p1 2F
85	1s2 2p2 (3P) 3d1	4F	1.5	9442168	70% + 11% 1s2 2p2 (3P) 3d1 4D
86	1s2 2p2 (3P) 3p1	4S	1.5	9460642	53% + 30% 1s2 2p2 (1D) 3p1 2P + 13% 1s2 2p2 (3P) 3p1 2P
87	1s2 2p2 (3P) 3d1	4F	2.5	9466629	58% + 24% 1s2 2p2 (3P) 3d1 4D
88	1s2 2p2 (3P) 3p1	4P	2.5	9472291	34% + 29% 1s2 2p2 (3P) 3p1 2D + 29% 1s2 2p2 (1D) 3p1 2F
89	1s2 2p2 (3P) 3p1	2P	1.5	9472381	47% + 23% 1s2 2p2 (3P) 3p1 4S + 11% 1s2 2p2 (3P) 3p1 4P
90	1s2 2p2 (3P) 3p1	2P	0.5	9504310	69% + 15% 1s2 2p2 (3P) 3p1 2S
91	1s2 2p2 (3P) 3d1	4F	3.5	9514316	75% + 21% 1s2 2p2 (3P) 3d1 4D
92	1s2 2p2 (3P) 3d1	2P	1.5	9516554	42% + 25% 1s2 2p2 (3P) 3d1 4D + 23% 1s2 2p2 (3P) 3d1 4F
93	1s2 2p2 (3P) 3d1	4F	2.5	9522857	32% + 26% 1s2 2p2 (3P) 3d1 2F + 20% 1s2 2p2 (1D) 3d1 2F
94	1s2 2p2 (3P) 3d1	4D	0.5	9525480	83% + 13% 1s2 2p2 (3P) 3d1 2P
95	1s2 2p2 (1D) 3p1	2F	2.5	9549139	49% + 24% 1s2 2p2 (1D) 3p1 2D + 15% 1s2 2p2 (3P) 3p1 2D
96	1s2 2p2 (3P) 3d1	4D	3.5	9551033	38% + 24% 1s2 2p2 (1D) 3d1 2F + 16% 1s2 2p2 (3P) 3d1 2F
97	1s2 2p2 (3P) 3d1	4F	4.5	9552660	82% + 18% 1s2 2p2 (1D) 3d1 2G
98	1s2 2p2 (3P) 3d1	4D	1.5	9555613	47% + 33% 1s2 2p2 (3P) 3d1 2P
99	1s2 2p2 (3P) 3d1	2F	2.5	9557712	32% + 26% 1s2 2p2 (3P) 3d1 4P + 22% 1s2 2p2 (3P) 3d1 4D
100	1s2 2p2 (1D) 3p1	2F	3.5	9563994	78% + 19% 1s2 2p2 (3P) 3p1 4D
101	1s2 2p2 (1D) 3p1	2D	1.5	9583303	48% + 22% 1s2 2p2 (1D) 3p1 2P + 14% 1s2 2p2 (3P) 3p1 2D
102	1s2 2p2 (1D) 3p1	2D	2.5	9597713	55% + 31% 1s2 2p2 (3P) 3p1 2D
103	1s2 2p2 (3P) 3d1	4P	2.5	9599924	48% + 31% 1s2 2p2 (3P) 3d1 4D + 16% 1s2 2p2 (1D) 3d1 2D
104	1s2 2p2 (1S) 3s1	2S	0.5	9602844	59% + 13% 1s2 2p2 (3P) 3d1 2P + 11% 1s2 2p2 (1D) 3d1 2S
105	1s2 2p2 (1D) 3p1	2P	0.5	9611964	89%
106	1s2 2p2 (3P) 3d1	4P	1.5	9613678	74%
107	1s2 2p2 (3P) 3d1	2P	0.5	9621528	49% + 24% 1s2 2p2 (1S) 3s1 2S + 16% 1s2 2p2 (3P) 3d1 4P
108	1s2 2p2 (3P) 3d1	4P	0.5	9624060	63% + 21% 1s2 2p2 (3P) 3d1 2P
109	1s2 2p2 (3P) 3d1	2F	3.5	9629317	36% + 29% 1s2 2p2 (1D) 3d1 2G + 28% 1s2 2p2 (3P) 3d1 4D
110	1s2 2p2 (3P) 3d1	2D	2.5	9667354	60% + 16% 1s2 2p2 (1D) 3d1 2F + 12% 1s2 2p2 (1D) 3d1 2D
111	1s2 2p2 (3P) 3d1	2D	1.5	9670700	71% + 12% 1s2 2p2 (1D) 3d1 2D
112	1s2 2p2 (1D) 3p1	2P	1.5	9683971	39% + 32% 1s2 2p2 (3P) 3p1 2P + 14% 1s2 2p2 (1D) 3p1 2D
113	1s2 2p2 (1D) 3d1	2G	3.5	9691641	45% + 39% 1s2 2p2 (1D) 3d1 2F + 11% 1s2 2p2 (3P) 3d1 4D
114	1s2 2p2 (1D) 3d1	2G	4.5	9708418	82% + 18% 1s2 2p2 (3P) 3d1 4F
115	1s2 2p2 (1D) 3d1	2D	1.5	9736179	73%
116	1s2 2p2 (1D) 3d1	2D	2.5	9740434	52% + 23% 1s2 2p2 (1D) 3d1 2F
117	1s2 2p2 (3P) 3d1	2F	3.5	9762003	40% + 36% 1s2 2p2 (1D) 3d1 2F + 17% 1s2 2p2 (1D) 3d1 2G
118	1s2 2p2 (1D) 3d1	2P	0.5	9763792	89%
119	1s2 2p2 (1S) 3p1	2P	0.5	9792303	84%
120	1s2 2p2 (3P) 3d1	2D	2.5	9801608	36% + 27% 1s2 2p2 (1D) 3d1 2F + 18% 1s2 2p2 (1D) 3d1 2D
121	1s2 2p2 (1D) 3d1	2S	0.5	9804009	80%
122	1s2 2p2 (1D) 3d1	2P	1.5	9806502	69% + 12% 1s2 2p2 (3P) 3d1 2P
123	1s2 2p2 (1S) 3p1	2P	1.5	9810603	86%
124	1s2 2p2 (1S) 3d1	2D	2.5	9960890	87%
125	1s2 2p2 (1S) 3d1	2D	1.5	9969426	83%
126	1s2 2s2 4s1	2S	0.5	10986106	95%
127	1s2 2s2 4p1	2P	0.5	11061237	95%
128	1s2 2s2 4p1	2P	1.5	11075121	95%
129	1s2 2s2 4d1	2D	1.5	11135585	95%
130	1s2 2s2 4d1	2D	2.5	11139649	95%
131	1s2 2s2 4f1	2F	2.5	11173539	95%
132	1s2 2s2 4f1	2F	3.5	11175356	95%
133	1s2 2s1 2p1 (3P) 4s1	4P	0.5	11340530	88% + 11% 1s2 2s1 2p1 (3P) 4s1 2P
134	1s2 2s1 2p1 (3P) 4s1	4P	1.5	11369374	86% + 11% 1s2 2s1 2p1 (3P) 4s1 2P
135	1s2 2s1 2p1 (3P) 4s1	2P	0.5	11389750	87% + 10% 1s2 2s1 2p1 (3P) 4s1 4P
136	1s2 2s1 2p1 (3P) 4p1	4D	0.5	11407650	74% + 19% 1s2 2s1 2p1 (3P) 4p1 2P
137	1s2 2s1 2p1 (3P) 4p1	4D	1.5	11428039	69% + 20% 1s2 2s1 2p1 (3P) 4p1 4P
138	1s2 2s1 2p1 (3P) 4p1	2P	1.5	11439838	33% + 22% 1s2 2s1 2p1 (3P) 4p1 4S + 17% 1s2 2s1 2p1 (3P) 4p1 4D
139	1s2 2s1 2p1 (3P) 4s1	4P	2.5	11457080	97%
140	1s2 2s1 2p1 (3P) 4p1	4P	0.5	11457418	81% + 13% 1s2 2s1 2p1 (3P) 4p1 2P
141	1s2 2s1 2p1 (3P) 4p1	4D	2.5	11457419	70% + 19% 1s2 2s1 2p1 (3P) 4p1 4P
142	1s2 2s1 2p1 (3P) 4p1	2P	0.5	11460571	49% + 23% 1s2 2s1 2p1 (3P) 4p1 4D + 21% 1s2 2s1 2p1 (3P) 4p1 2S
143	1s2 2s1 2p1 (3P) 4p1	2D	1.5	11470801	57% + 19% 1s2 2s1 2p1 (3P) 4p1 4S + 16% 1s2 2s1 2p1 (3P) 4p1 4P
144	1s2 2s1 2p1 (3P) 4d1	4F	1.5	11478339	76% + 10% 1s2 2s1 2p1 (3P) 4d1 4D
145	1s2 2s1 2p1 (3P) 4s1	2P	1.5	11481674	88% + 11% 1s2 2s1 2p1 (3P) 4s1 4P
146	1s2 2s1 2p1 (3P) 4d1	4F	2.5	11489897	51% + 28% 1s2 2s1 2p1 (3P) 4d1 4D + 12% 1s2 2s1 2p1 (3P) 4d1 4P
147	1s2 2s1 2p1 (3P) 4d1	4P	2.5	11511057	33% + 31% 1s2 2s1 2p1 (3P) 4d1 4F + 26% 1s2 2s1 2p1 (3P) 4d1 2D
148	1s2 2s1 2p1 (3P) 4d1	4F	3.5	11516474	62% + 29% 1s2 2s1 2p1 (3P) 4d1 4D
149	1s2 2s1 2p1 (3P) 4d1	4D	1.5	11518812	50% + 29% 1s2 2s1 2p1 (3P) 4d1 4P
150	1s2 2s1 2p1 (3P) 4d1	4D	0.5	11521977	81%
151	1s2 2s1 2p1 (3P) 4f1	4G	2.5	11522349	48% + 21% 1s2 2s1 2p1 (3P) 4f1 4F + 14% 1s2 2s1 2p1 (3P) 4f1 2F
152	1s2 2s1 2p1 (3P) 4f1	4F	3.5	11524662	30% + 22% 1s2 2s1 2p1 (3P) 4f1 4D + 20% 1s2 2s1 2p1 (3P) 4f1 4G
153	1s2 2s1 2p1 (3P) 4d1	2D	1.5	11534686	50% + 34% 1s2 2s1 2p1 (3P) 4d1 2P + 13% 1s2 2s1 2p1 (3P) 4d1 4F
154	1s2 2s1 2p1 (3P) 4p1	4P	1.5	11538763	43% + 23% 1s2 2s1 2p1 (3P) 4p1 2P + 16% 1s2 2s1 2p1 (3P) 4p1 4S
155	1s2 2s1 2p1 (3P) 4p1	4D	3.5	11539955	99%
156	1s2 2s1 2p1 (3P) 4d1	2F	2.5	11541402	59% + 15% 1s2 2s1 2p1 (3P) 4d1 4P + 15% 1s2 2s1 2p1 (3P) 4d1 2D
157	1s2 2s1 2p1 (3P) 4p1	4P	2.5	11542484	52% + 28% 1s2 2s1 2p1 (3P) 4p1 4D + 19% 1s2 2s1 2p1 (3P) 4p1 2D
158	1s2 2s1 2p1 (3P) 4p1	2P	1.5	11549509	35% + 33% 1s2 2s1 2p1 (3P) 4p1 4S + 12% 1s2 2s1 2p1 (3P) 4p1 2D
159	1s2 2s1 2p1 (3P) 4f1	4F	1.5	11551577	63% + 12% 1s2 2s1 2p1 (3P) 4f1 4D + 11% 1s2 2s1 2p1 (3P) 4f1 2D
160	1s2 2s1 2p1 (3P) 4f1	4G	3.5	11552614	44% + 33% 1s2 2s1 2p1 (3P) 4f1 2F + 11% 1s2 2s1 2p1 (3P) 4f1 2G
161	1s2 2s1 2p1 (3P) 4f1	4F	2.5	11553334	34% + 29% 1s2 2s1 2p1 (3P) 4f1 4D + 27% 1s2 2s1 2p1 (3P) 4f1 2F
162	1s2 2s1 2p1 (3P) 4f1	4G	4.5	11553358	43% + 41% 1s2 2s1 2p1 (3P) 4f1 4F + 14% 1s2 2s1 2p1 (3P) 4f1 2G
163	1s2 2s1 2p1 (3P) 4f1	2D	2.5	11558617	41% + 34% 1s2 2s1 2p1 (3P) 4f1 4G + 17% 1s2 2s1 2p1 (3P) 4f1 2F
164	1s2 2s1 2p1 (3P) 4f1	2G	3.5	11559897	44% + 38% 1s2 2s1 2p1 (3P) 4f1 4D
165	1s2 2s1 2p1 (3P) 4p1	2D	2.5	11566890	71% + 26% 1s2 2s1 2p1 (3P) 4p1 4P
166	1s2 2s1 2p1 (3P) 4p1	2S	0.5	11577839	71% + 16% 1s2 2s1 2p1 (3P) 4p1 2P
167	1s2 2s1 2p1 (3P) 4d1	4F	4.5	11596554	100%
168	1s2 2s1 2p1 (3P) 4d1	4D	3.5	11604622	63% + 35% 1s2 2s1 2p1 (3P) 4d1 4F
169	1s2 2s1 2p1 (3P) 4d1	4D	2.5	11607936	56% + 20% 1s2 2s1 2p1 (3P) 4d1 4P + 14% 1s2 2s1 2p1 (3P) 4d1 4F
170	1s2 2s1 2p1 (3P) 4d1	4P	1.5	11611137	61% + 36% 1s2 2s1 2p1 (3P) 4d1 4D
171	1s2 2s1 2p1 (3P) 4d1	4P	0.5	11612623	90%
172	1s2 2s1 2p1 (3P) 4d1	2D	2.5	11620801	50% + 25% 1s2 2s1 2p1 (3P) 4d1 2F + 17% 1s2 2s1 2p1 (3P) 4d1 4P
173	1s2 2s1 2p1 (3P) 4d1	2P	1.5	11632223	57% + 29% 1s2 2s1 2p1 (3P) 4d1 2D
174	1s2 2s1 2p1 (3P) 4d1	2F	3.5	11641117	91%
175	1s2 2s1 2p1 (3P) 4f1	4F	3.5	11642518	46% + 26% 1s2 2s1 2p1 (3P) 4f1 4G + 12% 1s2 2s1 2p1 (3P) 4f1 2F
176	1s2 2s1 2p1 (3P) 4f1	4F	4.5	11642764	54% + 46% 1s2 2s1 2p1 (3P) 4f1 4G
177	1s2 2s1 2p1 (3P) 4f1	4F	2.5	11644818	43% + 30% 1s2 2s1 2p1 (3P) 4f1 4D + 10% 1s2 2s1 2p1 (3P) 4f1 2D
178	1s2 2s1 2p1 (3P) 4f1	2F	3.5	11646915	46% + 23% 1s2 2s1 2p1 (3P) 4f1 4D + 18% 1s2 2s1 2p1 (3P) 4f1 2G
179	1s2 2s1 2p1 (3P) 4f1	4G	5.5	11646958	100%
180	1s2 2s1 2p1 (3P) 4d1	2P	0.5	11647548	90%
181	1s2 2s1 2p1 (3P) 4f1	4D	1.5	11648980	69% + 23% 1s2 2s1 2p1 (3P) 4f1 4F
182	1s2 2s1 2p1 (3P) 4f1	2G	4.5	11650991	85% + 10% 1s2 2s1 2p1 (3P) 4f1 4G
183	1s2 2s1 2p1 (3P) 4f1	4D	2.5	11651834	34% + 33% 1s2 2s1 2p1 (3P) 4f1 2D + 31% 1s2 2s1 2p1 (3P) 4f1 2F
184	1s2 2s1 2p1 (3P) 4f1	4D	0.5	11652069	100%
185	1s2 2s1 2p1 (3P) 4f1	2D	1.5	11657791	79% + 17% 1s2 2s1 2p1 (3P) 4f1 4D
186	1s2 2s1 2p1 (1P) 4s1	2P	0.5	11758032	96%
187	1s2 2s1 2p1 (1P) 4s1	2P	1.5	11759674	96%
188	1s2 2s1 2p1 (1P) 4p1	2D	1.5	11832259	82% + 14% 1s2 2s1 2p1 (1P) 4p1 2P
189	1s2 2s1 2p1 (1P) 4p1	2P	0.5	11833806	85% + 11% 1s2 2s1 2p1 (1P) 4p1 2S
190	1s2 2s1 2p1 (1P) 4p1	2D	2.5	11841574	96%
191	1s2 2s1 2p1 (1P) 4p1	2P	1.5	11847478	82% + 13% 1s2 2s1 2p1 (1P) 4p1 2D
192	1s2 2s1 2p1 (1P) 4p1	2S	0.5	11855186	83% + 11% 1s2 2s1 2p1 (1P) 4p1 2P
193	1s2 2s1 2p1 (1P) 4d1	2D	1.5	11902998	97%
194	1s2 2s1 2p1 (1P) 4d1	2F	2.5	11903215	91%
195	1s2 2s1 2p1 (1P) 4d1	2F	3.5	11903365	97%
196	1s2 2s1 2p1 (1P) 4d1	2D	2.5	11908277	91%
197	1s2 2s1 2p1 (1P) 4d1	2P	0.5	11916727	97%
198	1s2 2s1 2p1 (1P) 4d1	2P	1.5	11920666	96%
199	1s2 2s1 2p1 (1P) 4f1	2F	2.5	11932709	97%
200	1s2 2s1 2p1 (1P) 4f1	2F	3.5	11934584	97%
201	1s2 2s1 2p1 (1P) 4f1	2G	3.5	11941218	97%
202	1s2 2s1 2p1 (1P) 4f1	2G	4.5	11942845	97%
203	1s2 2s1 2p1 (1P) 4f1	2D	1.5	11948864	97%
204	1s2 2s1 2p1 (1P) 4f1	2D	2.5	11950454	97%
205	1s2 2p2 (3P) 4s1	4P	0.5	11966282	72% + 20% 1s2 2p2 (3P) 4s1 2P
206	1s2 2p2 (3P) 4p1	4D	0.5	12026218	57% + 13% 1s2 2p2 (3P) 4p1 2S + 13% 1s2 2p2 (3P) 4p1 2P
207	1s2 2p2 (3P) 4s1	4P	1.5	12032154	90%
208	1s2 2p2 (3P) 4s1	2P	0.5	12044766	75% + 23% 1s2 2p2 (3P) 4s1 4P
209	1s2 2p2 (3P) 4p1	4D	1.5	12048491	41% + 28% 1s2 2p2 (3P) 4p1 4P + 16% 1s2 2p2 (3P) 4p1 2D
210	1s2 2p2 (3P) 4s1	4P	2.5	12077037	74% + 22% 1s2 2p2 (1D) 4s1 2D
211	1s2 2p2 (3P) 4p1	2S	0.5	12090712	36% + 32% 1s2 2p2 (3P) 4p1 4D + 32% 1s2 2p2 (3P) 4p1 4P
212	1s2 2p2 (3P) 4d1	4F	1.5	12091037	31% + 27% 1s2 2p2 (3P) 4s1 2P + 12% 1s2 2p2 (1D) 4s1 2D
213	1s2 2p2 (3P) 4s1	2P	1.5	12096944	38% + 24% 1s2 2p2 (3P) 4d1 4F + 16% 1s2 2p2 (1D) 4s1 2D
214	1s2 2p2 (3P) 4p1	4D	1.5	12104155	51% + 14% 1s2 2p2 (3P) 4p1 2D + 12% 1s2 2p2 (3P) 4p1 2P
215	1s2 2p2 (3P) 4d1	4F	2.5	12109479	33% + 28% 1s2 2p2 (3P) 4d1 4D + 15% 1s2 2p2 (3P) 4d1 2F
216	1s2 2p2 (3P) 4p1	4D	2.5	12109603	68% + 24% 1s2 2p2 (3P) 4p1 4P
217	1s2 2p2 (3P) 4p1	4P	0.5	12119410	50% + 23% 1s2 2p2 (3P) 4p1 2P + 20% 1s2 2p2 (3P) 4p1 2S
218	1s2 2p2 (3P) 4p1	2D	1.5	12125947	58% + 23% 1s2 2p2 (3P) 4p1 4P + 15% 1s2 2p2 (3P) 4p1 4S
219	1s2 2p2 (3P) 4f1	4G	2.5	12133488	43% + 17% 1s2 2p2 (3P) 4f1 2D + 15% 1s2 2p2 (3P) 4f1 4F
220	1s2 2p2 (3P) 4f1	4D	3.5	12136390	24% + 23% 1s2 2p2 (3P) 4f1 2G + 21% 1s2 2p2 (3P) 4f1 4F
221	1s2 2p2 (3P) 4p1	4P	2.5	12142023	31% + 22% 1s2 2p2 (3P) 4p1 4D + 19% 1s2 2p2 (3P) 4p1 2D
222	1s2 2p2 (3P) 4p1	4D	3.5	12153226	77% + 23% 1s2 2p2 (1D) 4p1 2F
223	1s2 2p2 (3P) 4p1	4S	1.5	12163250	50% + 26% 1s2 2p2 (3P) 4p1 4P + 16% 1s2 2p2 (1D) 4p1 2P
224	1s2 2p2 (3P) 4d1	4F	1.5	12165218	36% + 35% 1s2 2p2 (3P) 4d1 2P + 18% 1s2 2p2 (3P) 4d1 4D
225	1s2 2p2 (3P) 4d1	4F	3.5	12167484	59% + 33% 1s2 2p2 (3P) 4d1 4D
226	1s2 2p2 (3P) 4d1	4D	0.5	12168370	80% + 14% 1s2 2p2 (3P) 4d1 2P
227	1s2 2p2 (3P) 4p1	2P	1.5	12170620	58% + 22% 1s2 2p2 (1D) 4p1 2D
228	1s2 2p2 (3P) 4d1	4F	2.5	12172277	56% + 23% 1s2 2p2 (3P) 4d1 4P
229	1s2 2p2 (3P) 4p1	2D	2.5	12179277	45% + 27% 1s2 2p2 (3P) 4p1 4P + 18% 1s2 2p2 (1D) 4p1 2F
230	1s2 2p2 (3P) 4p1	2P	0.5	12185339	57% + 22% 1s2 2p2 (3P) 4p1 2S + 11% 1s2 2p2 (1D) 4p1 2P
231	1s2 2p2 (3P) 4d1	4D	1.5	12186252	37% + 28% 1s2 2p2 (3P) 4d1 2P + 17% 1s2 2p2 (3P) 4d1 2D
232	1s2 2p2 (3P) 4d1	2F	2.5	12187456	64% + 21% 1s2 2p2 (3P) 4d1 4P
233	1s2 2p2 (3P) 4f1	4G	2.5	12200490	44% + 35% 1s2 2p2 (3P) 4f1 2D + 15% 1s2 2p2 (3P) 4f1 4D
234	1s2 2p2 (3P) 4f1	4D	3.5	12202351	44% + 42% 1s2 2p2 (3P) 4f1 4G
235	1s2 2p2 (3P) 4f1	4G	4.5	12205379	53% + 31% 1s2 2p2 (3P) 4f1 4F + 16% 1s2 2p2 (3P) 4f1 2G
236	1s2 2p2 (3P) 4f1	2G	3.5	12205809	52% + 18% 1s2 2p2 (3P) 4f1 4G + 15% 1s2 2p2 (3P) 4f1 2F
237	1s2 2p2 (3P) 4f1	4F	1.5	12206952	59% + 21% 1s2 2p2 (3P) 4f1 4D + 20% 1s2 2p2 (3P) 4f1 2D
238	1s2 2p2 (3P) 4d1	4D	3.5	12207587	32% + 29% 1s2 2p2 (3P) 4d1 4F + 17% 1s2 2p2 (1D) 4d1 2F
239	1s2 2p2 (3P) 4d1	4F	4.5	12209498	78% + 22% 1s2 2p2 (1D) 4d1 2G
240	1s2 2p2 (3P) 4f1	2F	2.5	12210388	30% + 29% 1s2 2p2 (3P) 4f1 4D + 24% 1s2 2p2 (3P) 4f1 4F
241	1s2 2p2 (1D) 4s1	2D	2.5	12213901	56% + 17% 1s2 2p2 (3P) 4s1 4P
242	1s2 2p2 (1D) 4s1	2D	1.5	12221564	68% + 24% 1s2 2p2 (3P) 4s1 2P
243	1s2 2p2 (3P) 4d1	4D	2.5	12222169	37% + 18% 1s2 2p2 (3P) 4d1 4P
244	1s2 2p2 (3P) 4d1	4P	1.5	12227306	57% + 19% 1s2 2p2 (3P) 4d1 4D + 13% 1s2 2p2 (1D) 4d1 2P
245	1s2 2p2 (3P) 4d1	4P	0.5	12230405	72% + 17% 1s2 2p2 (1D) 4d1 2S
246	1s2 2p2 (3P) 4d1	2P	0.5	12236303	68% + 14% 1s2 2p2 (3P) 4d1 4D + 11% 1s2 2p2 (1D) 4d1 2P
247	1s2 2p2 (3P) 4d1	2F	3.5	12243343	54% + 21% 1s2 2p2 (1D) 4d1 2G + 18% 1s2 2p2 (3P) 4d1 4D
248	1s2 2p2 (3P) 4d1	2D	1.5	12244386	58% + 15% 1s2 2p2 (1D) 4d1 2D + 10% 1s2 2p2 (3P) 4d1 2P
249	1s2 2p2 (3P) 4d1	2D	2.5	12244441	53% + 19% 1s2 2p2 (1D) 4d1 2F
250	1s2 2p2 (3P) 4f1	4G	4.5	12248830	32% + 31% 1s2 2p2 (3P) 4f1 2G + 18% 1s2 2p2 (1D) 4f1 2H
251	1s2 2p2 (3P) 4f1	4G	5.5	12249213	77% + 23% 1s2 2p2 (1D) 4f1 2H
252	1s2 2p2 (3P) 4f1	4D	0.5	12251273	79% + 20% 1s2 2p2 (1D) 4f1 2P
253	1s2 2p2 (3P) 4f1	4F	3.5	12251580	42% + 19% 1s2 2p2 (1D) 4f1 2G + 13% 1s2 2p2 (3P) 4f1 4G
254	1s2 2p2 (3P) 4f1	4D	1.5	12251859	61% + 15% 1s2 2p2 (3P) 4f1 4F + 11% 1s2 2p2 (1D) 4f1 2P
255	1s2 2p2 (3P) 4f1	4F	2.5	12252205	42% + 26% 1s2 2p2 (3P) 4f1 4D + 18% 1s2 2p2 (1D) 4f1 2F
256	1s2 2p2 (3P) 4f1	4F	4.5	12254349	38% + 32% 1s2 2p2 (3P) 4f1 2G + 21% 1s2 2p2 (1D) 4f1 2G
257	1s2 2p2 (3P) 4f1	2D	1.5	12254654	60% + 17% 1s2 2p2 (3P) 4f1 4F + 12% 1s2 2p2 (1D) 4f1 2D
258	1s2 2p2 (3P) 4f1	2F	3.5	12255378	43% + 19% 1s2 2p2 (1D) 4f1 2F + 11% 1s2 2p2 (3P) 4f1 4D
259	1s2 2p2 (3P) 4f1	2F	2.5	12255749	42% + 19% 1s2 2p2 (3P) 4f1 2D + 16% 1s2 2p2 (1D) 4f1 2D
260	1s2 2s2 5s1	2S	0.5	12279291	95%
261	1s2 2p2 (1D) 4p1	2F	2.5	12289009	53% + 20% 1s2 2p2 (1D) 4p1 2D + 19% 1s2 2p2 (3P) 4p1 2D
262	1s2 2p2 (1D) 4p1	2D	1.5	12293068	45% + 30% 1s2 2p2 (1D) 4p1 2P
263	1s2 2p2 (1D) 4p1	2F	3.5	12294467	76% + 23% 1s2 2p2 (3P) 4p1 4D
264	1s2 2p2 (1D) 4p1	2D	2.5	12295436	58% + 15% 1s2 2p2 (1D) 4p1 2F + 11% 1s2 2p2 (3P) 4p1 4P
265	1s2 2p2 (1D) 4p1	2P	0.5	12303528	84%
266	1s2 2s2 5p1	2P	0.5	12315762	95%
267	1s2 2s2 5p1	2P	1.5	12322749	95%
268	1s2 2p2 (1D) 4p1	2P	1.5	12331975	42% + 23% 1s2 2p2 (1D) 4p1 2D + 21% 1s2 2p2 (3P) 4p1 2P
269	1s2 2p2 (1D) 4d1	2F	3.5	12345098	53% + 24% 1s2 2p2 (1D) 4d1 2G + 13% 1s2 2p2 (3P) 4d1 4D
270	1s2 2s2 5d1	2D	1.5	12351697	95%
271	1s2 2p2 (1D) 4d1	2G	4.5	12352563	77% + 22% 1s2 2p2 (3P) 4d1 4F
272	1s2 2s2 5d1	2D	2.5	12353856	95%
273	1s2 2p2 (1D) 4d1	2D	2.5	12359613	47% + 27% 1s2 2p2 (1D) 4d1 2F + 12% 1s2 2p2 (3P) 4d1 4D
274	1s2 2p2 (1D) 4d1	2D	1.5	12360467	69%
275	1s2 2p2 (1D) 4d1	2G	3.5	12362665	44% + 25% 1s2 2p2 (1D) 4d1 2F + 18% 1s2 2p2 (3P) 4d1 2F
276	1s2 2p2 (1D) 4d1	2P	0.5	12364441	79%
277	1s2 2s2 5f1	2F	2.5	12370344	95%
278	1s2 2s2 5f1	2F	3.5	12371272	95%
279	1s2 2s2 5g1	2G	3.5	12374527	95%
280	1s2 2s2 5g1	2G	4.5	12375073	95%
281	1s2 2p2 (1D) 4d1	2S	0.5	12379477	72% + 16% 1s2 2p2 (3P) 4d1 4P
282	1s2 2p2 (1D) 4d1	2F	2.5	12380298	36% + 26% 1s2 2p2 (1D) 4d1 2D + 24% 1s2 2p2 (3P) 4d1 2D
283	1s2 2p2 (1D) 4f1	2G	4.5	12383167	72% + 19% 1s2 2p2 (3P) 4f1 4F
284	1s2 2p2 (1D) 4f1	2G	3.5	12383475	56% + 15% 1s2 2p2 (1D) 4f1 2F + 12% 1s2 2p2 (3P) 4f1 4F
285	1s2 2p2 (1D) 4f1	2F	2.5	12385035	70% + 11% 1s2 2p2 (3P) 4f1 4F
286	1s2 2p2 (1D) 4d1	2P	1.5	12385131	68%
287	1s2 2p2 (1D) 4f1	2F	3.5	12387472	57% + 14% 1s2 2p2 (1D) 4f1 2G + 13% 1s2 2p2 (3P) 4f1 2F
288	1s2 2p2 (1D) 4f1	2H	4.5	12389246	76% + 17% 1s2 2p2 (3P) 4f1 2G
289	1s2 2p2 (1D) 4f1	2H	5.5	12390193	77% + 23% 1s2 2p2 (3P) 4f1 4G
290	1s2 2p2 (1D) 4f1	2D	1.5	12391428	76%
291	1s2 2p2 (1D) 4f1	2D	2.5	12394627	74% + 10% 1s2 2p2 (3P) 4f1 4D
292	1s2 2p2 (1D) 4f1	2P	0.5	12399188	79% + 20% 1s2 2p2 (3P) 4f1 4D
293	1s2 2p2 (1D) 4f1	2P	1.5	12400743	79% + 11% 1s2 2p2 (3P) 4f1 2D
294	1s2 2p2 (1S) 4s1	2S	0.5	12444475	86%
295	1s2 2p2 (1S) 4p1	2P	0.5	12515791	88%
296	1s2 2p2 (1S) 4p1	2P	1.5	12525285	89%
297	1s2 2p2 (1S) 4d1	2D	2.5	12584193	89%
298	1s2 2p2 (1S) 4d1	2D	1.5	12585234	88%
299	1s2 2p2 (1S) 4f1	2F	2.5	12612343	89%
300	1s2 2p2 (1S) 4f1	2F	3.5	12613762	89%
301	1s2 2s1 2p1 (3P) 5s1	4P	0.5	12630518	80% + 20% 1s2 2s1 2p1 (3P) 5s1 2P
302	1s2 2s1 2p1 (3P) 5s1	4P	1.5	12659932	84% + 13% 1s2 2s1 2p1 (3P) 5s1 2P
303	1s2 2s1 2p1 (3P) 5p1	4D	0.5	12664345	68% + 20% 1s2 2s1 2p1 (3P) 5p1 2P
304	1s2 2s1 2p1 (3P) 5s1	2P	0.5	12668513	78% + 19% 1s2 2s1 2p1 (3P) 5s1 4P
305	1s2 2s1 2p1 (3P) 5p1	4D	1.5	12674610	39% + 29% 1s2 2s1 2p1 (3P) 5p1 4P + 18% 1s2 2s1 2p1 (3P) 5p1 2D
306	1s2 2s1 2p1 (3P) 5p1	4D	1.5	12694215	46% + 27% 1s2 2s1 2p1 (3P) 5p1 2P + 13% 1s2 2s1 2p1 (3P) 5p1 4S
307	1s2 2s1 2p1 (3P) 5d1	4F	1.5	12699708	65% + 14% 1s2 2s1 2p1 (3P) 5d1 4D + 12% 1s2 2s1 2p1 (3P) 5d1 2D
308	1s2 2s1 2p1 (3P) 5p1	4P	0.5	12702390	79%
309	1s2 2s1 2p1 (3P) 5p1	4D	2.5	12704007	63% + 23% 1s2 2s1 2p1 (3P) 5p1 4P + 12% 1s2 2s1 2p1 (3P) 5p1 2D
310	1s2 2s1 2p1 (3P) 5d1	4F	2.5	12705133	31% + 30% 1s2 2s1 2p1 (3P) 5d1 4D + 21% 1s2 2s1 2p1 (3P) 5d1 4P
311	1s2 2s1 2p1 (3P) 5p1	2P	0.5	12706122	52% + 24% 1s2 2s1 2p1 (3P) 5p1 4D + 21% 1s2 2s1 2p1 (3P) 5p1 2S
312	1s2 2s1 2p1 (3P) 5p1	2D	1.5	12709631	56% + 20% 1s2 2s1 2p1 (3P) 5p1 4S + 19% 1s2 2s1 2p1 (3P) 5p1 4P
313	1s2 2s1 2p1 (3P) 5f1	4G	2.5	12719581	47% + 20% 1s2 2s1 2p1 (3P) 5f1 4F + 15% 1s2 2s1 2p1 (3P) 5f1 2D
314	1s2 2s1 2p1 (3P) 5f1	4F	3.5	12720793	28% + 24% 1s2 2s1 2p1 (3P) 5f1 4D + 22% 1s2 2s1 2p1 (3P) 5f1 2G
315	1s2 2s1 2p1 (3P) 5g1	4H	3.5	12723256	41% + 20% 1s2 2s1 2p1 (3P) 5g1 4G + 18% 1s2 2s1 2p1 (3P) 5g1 2F
316	1s2 2s1 2p1 (3P) 5g1	4G	4.5	12723812	25% + 25% 1s2 2s1 2p1 (3P) 5g1 4F + 25% 1s2 2s1 2p1 (3P) 5g1 2H
317	1s2 2s1 2p1 (3P) 5d1	4F	2.5	12729171	49% + 24% 1s2 2s1 2p1 (3P) 5d1 2D + 23% 1s2 2s1 2p1 (3P) 5d1 4P
318	1s2 2s1 2p1 (3P) 5d1	4D	1.5	12733531	44% + 29% 1s2 2s1 2p1 (3P) 5d1 4P + 11% 1s2 2s1 2p1 (3P) 5d1 4F
319	1s2 2s1 2p1 (3P) 5d1	4F	3.5	12733667	55% + 32% 1s2 2s1 2p1 (3P) 5d1 4D + 11% 1s2 2s1 2p1 (3P) 5d1 2F
320	1s2 2s1 2p1 (3P) 5d1	4D	0.5	12735488	77% + 12% 1s2 2s1 2p1 (3P) 5d1 2P
321	1s2 2s1 2p1 (3P) 5d1	2D	1.5	12740788	40% + 38% 1s2 2s1 2p1 (3P) 5d1 2P + 18% 1s2 2s1 2p1 (3P) 5d1 4F
322	1s2 2s1 2p1 (3P) 5d1	2F	2.5	12743266	59% + 18% 1s2 2s1 2p1 (3P) 5d1 4P
323	1s2 2s1 2p1 (3P) 5f1	4F	1.5	12749823	68% + 15% 1s2 2s1 2p1 (3P) 5f1 4D + 14% 1s2 2s1 2p1 (3P) 5f1 2D
324	1s2 2s1 2p1 (3P) 5f1	4G	3.5	12750182	49% + 29% 1s2 2s1 2p1 (3P) 5f1 2F
325	1s2 2s1 2p1 (3P) 5f1	4G	4.5	12750617	44% + 38% 1s2 2s1 2p1 (3P) 5f1 4F + 15% 1s2 2s1 2p1 (3P) 5f1 2G
326	1s2 2s1 2p1 (3P) 5f1	4D	2.5	12750624	33% + 32% 1s2 2s1 2p1 (3P) 5f1 4F + 23% 1s2 2s1 2p1 (3P) 5f1 2F
327	1s2 2s1 2p1 (3P) 5s1	4P	2.5	12750970	96%
328	1s2 2s1 2p1 (3P) 5f1	2D	2.5	12753515	44% + 33% 1s2 2s1 2p1 (3P) 5f1 4G + 19% 1s2 2s1 2p1 (3P) 5f1 2F
329	1s2 2s1 2p1 (3P) 5g1	4H	4.5	12753912	38% + 30% 1s2 2s1 2p1 (3P) 5g1 2G + 20% 1s2 2s1 2p1 (3P) 5g1 2H
330	1s2 2s1 2p1 (3P) 5f1	2G	3.5	12753933	47% + 37% 1s2 2s1 2p1 (3P) 5f1 4D
331	1s2 2s1 2p1 (3P) 5g1	4G	2.5	12753995	62% + 19% 1s2 2s1 2p1 (3P) 5g1 4F + 15% 1s2 2s1 2p1 (3P) 5g1 2F
332	1s2 2s1 2p1 (3P) 5g1	4H	5.5	12754416	42% + 40% 1s2 2s1 2p1 (3P) 5g1 4G + 16% 1s2 2s1 2p1 (3P) 5g1 2H
333	1s2 2s1 2p1 (3P) 5g1	2G	3.5	12754525	33% + 31% 1s2 2s1 2p1 (3P) 5g1 4F + 27% 1s2 2s1 2p1 (3P) 5g1 4G
334	1s2 2s1 2p1 (3P) 5g1	4H	3.5	12755347	46% + 41% 1s2 2s1 2p1 (3P) 5g1 2F
335	1s2 2s1 2p1 (3P) 5g1	4F	4.5	12755830	47% + 32% 1s2 2s1 2p1 (3P) 5g1 2H + 15% 1s2 2s1 2p1 (3P) 5g1 4H
336	1s2 2s1 2p1 (3P) 5s1	2P	1.5	12761021	86% + 14% 1s2 2s1 2p1 (3P) 5s1 4P
337	1s2 2s1 2p1 (3P) 5p1	4P	1.5	12789953	43% + 22% 1s2 2s1 2p1 (3P) 5p1 4S + 19% 1s2 2s1 2p1 (3P) 5p1 2P
338	1s2 2s1 2p1 (3P) 5p1	4P	2.5	12791181	46% + 36% 1s2 2s1 2p1 (3P) 5p1 4D + 18% 1s2 2s1 2p1 (3P) 5p1 2D
339	1s2 2s1 2p1 (3P) 5p1	4D	3.5	12791466	100%
340	1s2 2s1 2p1 (3P) 5p1	2P	1.5	12796141	48% + 33% 1s2 2s1 2p1 (3P) 5p1 4S + 12% 1s2 2s1 2p1 (3P) 5p1 2D
341	1s2 2s1 2p1 (3P) 5p1	2D	2.5	12803110	69% + 30% 1s2 2s1 2p1 (3P) 5p1 4P
342	1s2 2s1 2p1 (3P) 5p1	2S	0.5	12808123	64% + 22% 1s2 2s1 2p1 (3P) 5p1 2P + 11% 1s2 2s1 2p1 (3P) 5p1 4P
343	1s2 2s1 2p1 (3P) 5d1	4F	4.5	12819666	100%
344	1s2 2s1 2p1 (3P) 5d1	4D	3.5	12822836	58% + 40% 1s2 2s1 2p1 (3P) 5d1 4F
345	1s2 2s1 2p1 (3P) 5d1	4D	2.5	12824275	55% + 17% 1s2 2s1 2p1 (3P) 5d1 4P + 17% 1s2 2s1 2p1 (3P) 5d1 4F
346	1s2 2s1 2p1 (3P) 5d1	4P	1.5	12825800	58% + 38% 1s2 2s1 2p1 (3P) 5d1 4D
347	1s2 2s1 2p1 (3P) 5d1	4P	0.5	12826522	89% + 10% 1s2 2s1 2p1 (3P) 5d1 4D
348	1s2 2s1 2p1 (3P) 5d1	2D	2.5	12830199	54% + 20% 1s2 2s1 2p1 (3P) 5d1 2F + 19% 1s2 2s1 2p1 (3P) 5d1 4P
349	1s2 2s1 2p1 (3P) 5d1	2P	1.5	12835076	48% + 36% 1s2 2s1 2p1 (3P) 5d1 2D + 10% 1s2 2s1 2p1 (3P) 5d1 4P
350	1s2 2s1 2p1 (3P) 5d1	2F	3.5	12838918	87%
351	1s2 2s1 2p1 (3P) 5f1	4F	3.5	12841180	52% + 24% 1s2 2s1 2p1 (3P) 5f1 4G + 12% 1s2 2s1 2p1 (3P) 5f1 4D
352	1s2 2s1 2p1 (3P) 5f1	4F	4.5	12841237	55% + 45% 1s2 2s1 2p1 (3P) 5f1 4G
353	1s2 2s1 2p1 (3P) 5f1	4F	2.5	12842245	46% + 32% 1s2 2s1 2p1 (3P) 5f1 4D
354	1s2 2s1 2p1 (3P) 5d1	2P	0.5	12842361	87% + 10% 1s2 2s1 2p1 (3P) 5d1 4D
355	1s2 2s1 2p1 (3P) 5f1	4G	5.5	12843058	100%
356	1s2 2s1 2p1 (3P) 5f1	2F	3.5	12843675	52% + 19% 1s2 2s1 2p1 (3P) 5f1 2G + 19% 1s2 2s1 2p1 (3P) 5f1 4D
357	1s2 2s1 2p1 (3P) 5f1	4D	1.5	12844088	70% + 25% 1s2 2s1 2p1 (3P) 5f1 4F
358	1s2 2s1 2p1 (3P) 5f1	4D	0.5	12845515	100%
359	1s2 2s1 2p1 (3P) 5g1	2G	4.5	12845612	30% + 29% 1s2 2s1 2p1 (3P) 5g1 4G + 28% 1s2 2s1 2p1 (3P) 5g1 4H
360	1s2 2s1 2p1 (3P) 5f1	2G	4.5	12845829	85%
361	1s2 2s1 2p1 (3P) 5f1	2F	2.5	12845954	36% + 33% 1s2 2s1 2p1 (3P) 5f1 2D + 28% 1s2 2s1 2p1 (3P) 5f1 4D
362	1s2 2s1 2p1 (3P) 5g1	4G	3.5	12845979	42% + 20% 1s2 2s1 2p1 (3P) 5g1 2G + 15% 1s2 2s1 2p1 (3P) 5g1 2F
363	1s2 2s1 2p1 (3P) 5g1	4G	5.5	12846054	57% + 40% 1s2 2s1 2p1 (3P) 5g1 4H
364	1s2 2s1 2p1 (3P) 5g1	4G	4.5	12846473	32% + 30% 1s2 2s1 2p1 (3P) 5g1 2G + 25% 1s2 2s1 2p1 (3P) 5g1 4F
365	1s2 2s1 2p1 (3P) 5g1	2H	5.5	12846865	81% + 17% 1s2 2s1 2p1 (3P) 5g1 4H
366	1s2 2s1 2p1 (3P) 5g1	4F	2.5	12847101	45% + 35% 1s2 2s1 2p1 (3P) 5g1 4G + 20% 1s2 2s1 2p1 (3P) 5g1 2F
367	1s2 2s1 2p1 (3P) 5g1	4H	6.5	12847235	100%
368	1s2 2s1 2p1 (3P) 5g1	4F	3.5	12847598	43% + 27% 1s2 2s1 2p1 (3P) 5g1 2G + 21% 1s2 2s1 2p1 (3P) 5g1 2F
369	1s2 2s1 2p1 (3P) 5g1	4F	1.5	12848351	100%
370	1s2 2s1 2p1 (3P) 5g1	2F	2.5	12848953	64% + 35% 1s2 2s1 2p1 (3P) 5g1 4F
371	1s2 2s1 2p1 (3P) 5f1	2D	1.5	12849038	80% + 15% 1s2 2s1 2p1 (3P) 5f1 4D
372	1s2 2s2 6s1	2S	0.5	12966803	94%
373	1s2 2s2 6p1	2P	0.5	12988610	94%
374	1s2 2s2 6p1	2P	1.5	12992885	94%
375	1s2 2s2 6d1	2D	1.5	13010344	95%
376	1s2 2s2 6d1	2D	2.5	13011577	95%
377	1s2 2s2 6f1	2F	2.5	13020767	95%
378	1s2 2s2 6f1	2F	3.5	13021353	96%
379	1s2 2s2 6h1	2H	4.5	13022298	95%
380	1s2 2s2 6g1	2G	3.5	13022462	95%
381	1s2 2s2 6h1	2H	5.5	13022514	95%
382	1s2 2s2 6g1	2G	4.5	13022792	95%
383	1s2 2s1 2p1 (1P) 5s1	2P	0.5	13048296	96%
384	1s2 2s1 2p1 (1P) 5s1	2P	1.5	13048997	96%
385	1s2 2s1 2p1 (1P) 5p1	2D	1.5	13084306	82% + 14% 1s2 2s1 2p1 (1P) 5p1 2P
386	1s2 2s1 2p1 (1P) 5p1	2P	0.5	13085077	89%
387	1s2 2s1 2p1 (1P) 5p1	2D	2.5	13089534	97%
388	1s2 2s1 2p1 (1P) 5p1	2P	1.5	13091712	83% + 14% 1s2 2s1 2p1 (1P) 5p1 2D
389	1s2 2s1 2p1 (1P) 5p1	2S	0.5	13097616	87%
390	1s2 2s1 2p1 (1P) 5d1	2D	1.5	13119131	97%
391	1s2 2s1 2p1 (1P) 5d1	2F	2.5	13119873	88%
392	1s2 2s1 2p1 (1P) 5d1	2F	3.5	13120241	97%
393	1s2 2s1 2p1 (1P) 5d1	2D	2.5	13121768	88%
394	1s2 2s1 2p1 (1P) 5d1	2P	0.5	13126394	97%
395	1s2 2s1 2p1 (1P) 5d1	2P	1.5	13128371	97%
396	1s2 2s1 2p1 (1P) 5f1	2F	2.5	13133808	97%
397	1s2 2s1 2p1 (1P) 5f1	2F	3.5	13134781	97%
398	1s2 2s1 2p1 (1P) 5g1	2G	3.5	13138485	97%
399	1s2 2s1 2p1 (1P) 5f1	2G	3.5	13138756	97%
400	1s2 2s1 2p1 (1P) 5g1	2G	4.5	13139009	97%
401	1s2 2s1 2p1 (1P) 5f1	2G	4.5	13139549	97%
402	1s2 2s1 2p1 (1P) 5f1	2D	1.5	13141514	97%
403	1s2 2s1 2p1 (1P) 5f1	2D	2.5	13142299	97%
404	1s2 2s1 2p1 (1P) 5g1	2H	4.5	13142538	96%
405	1s2 2s1 2p1 (1P) 5g1	2H	5.5	13143067	97%
406	1s2 2s1 2p1 (1P) 5g1	2F	2.5	13143102	97%
407	1s2 2s1 2p1 (1P) 5g1	2F	3.5	13143620	97%

   

Table 2: Suggested change of spectroscopic identifications of levels to ensure the completeness of spectroscopic dataset. The indices of levels for which spectroscopic identifications are changed are presented in the first column. The second column contains index of level with the same highest contribution of configuration state function (Table 1) as level from the first column before change. Indices of levels in the first two columns are taken from Table 1.

Index	Index	Changed CSF
88	81	2p2 (3P) 3p1 2D2.5
87	93	2p2 (3P) 3d1 4D2.5
117	109	2p2 (1D) 3d1 2F3.5
120	110	2p2 (1D) 3d1 2F2.5
152	175	2s1 2p1 (3P) 4f1 4D3.5
161	177	2s1 2p1 (3P) 4f1 2F2.5
209	214	2p2 (3P) 4p1 4P1.5
224	213	2p2 (3P) 4d1 2P1.5
228	215	2p2 (3P) 4d1 4P2.5
219	233	2p2 (3P) 4f1 2D2.5
234	220	2p2 (3P) 4f1 4G3.5
306	305	2s1 2p1 (3P) 5p1 4S1.5
310	317	2s1 2p1 (3P) 5d1 4P2.5
314	351	2s1 2p1 (3P) 5f1 4D3.5
315	334	2s1 2p1 (3P) 5g1 2F3.5
316	364	2s1 2p1 (3P) 5g1 2H4.5

   

Table 3: Comparison of calculated energies  $E^{{\rm GRASP}}$ and  $E^{{\rm CITRO}}$ for Fe XXII levels with data compiled by NIST ( $E^{{\rm NIST}}$). Indices of levels in the first column and CSFs in the second column are taken from Table 1. Energies are in cm^-1. The lifetimes of levels are presented in the last two columns.

Index	CSF	$E^{{\rm NIST}}$	$E^{{\rm CITRO}}$	$E^{{\rm GRASP}}$	$\tau^{{\rm CITRO}}$ (s)	$\tau^{{\rm GRASP}}$ (s)
2	1s2 2s2 2p1 2P1.5	118266	115650	117953	7.19E-05	6.81E-05
3	1s2 2s1 2p2 4P0.5	404550	399846	402902	1.06E-08	1.09E-08
4	1s2 2s1 2p2 4P1.5	460190	454430	458031	9.81E-08	1.02E-07
5	1s2 2s1 2p2 4P2.5	513260	506869	511295	1.41E-08	1.48E-08
6	1s2 2s1 2p2 2D1.5	736310	728951	741538	9.49E-11	9.13E-11
7	1s2 2s1 2p2 2D2.5	759210	751725	763743	1.71E-10	1.65E-10
8	1s2 2s1 2p2 2P0.5	853650	847120	861921	2.64E-11	2.55E-11
9	1s2 2s1 2p2 2S0.5	978350	969456	986277	2.82E-11	2.71E-11
10	1s2 2s1 2p2 2P1.5	992320	983323	1000692	2.01E-11	1.94E-11
11	1s2 2p3 4S1.5	1255700	1245542	1260179	2.29E-11	2.22E-11
12	1s2 2p3 2D1.5	1396110	1384720	1405688	4.69E-11	4.61E-11
13	1s2 2p3 2D2.5	1426570	1414255	1435674	4.89E-11	4.77E-11
14	1s2 2p3 2P0.5	1569630	1556753	1582452	2.33E-11	2.24E-11
15	1s2 2p3 2P1.5	1627720	1613294	1639226	2.38E-11	2.30E-11
20	1s2 2s2 3d1 2D1.5	8498000	8508732	8491152	5.10E-14	5.12E-14
21	1s2 2s2 3d1 2D2.5	8507000	8518565	8501013	5.26E-14	5.31E-14
28	1s2 2s1 2p1 (3P) 3p1 2P1.5	8688000	8707856	8695560	2.85E-13	2.96E-13
29	1s2 2s1 2p1 (3P) 3p1 2P0.5	8584000	8716292	8704356	1.35E-13	1.38E-13
32	1s2 2s1 2p1 (3P) 3p1 2D1.5	8740000	8758943	8748534	1.94E-13	1.99E-13
39	1s2 2s1 2p1 (3P) 3p1 2D2.5	8845000	8862704	8857624	1.30E-13	1.35E-13
40	1s2 2s1 2p1 (3P) 3d1 4F3.5	8864000	8870786	8857700	1.68E-13	1.64E-13
41	1s2 2s1 2p1 (3P) 3d1 4P2.5	8874000	8882016	8868503	5.84E-14	5.93E-14
42	1s2 2s1 2p1 (3P) 3d1 4D1.5	8882000	8890791	8878309	5.97E-14	4.23E-14
43	1s2 2s1 2p1 (3P) 3d1 4D0.5	8888000	8895387	8881447	3.73E-14	3.52E-14
49	1s2 2s1 2p1 (3P) 3d1 2D2.5	8938000	8940836	8930222	6.80E-14	6.84E-14
50	1s2 2s1 2p1 (3P) 3d1 4D3.5	8962000	8965402	8955370	4.06E-14	4.13E-14
51	1s2 2s1 2p1 (3P) 3d1 4D2.5	8973000	8976048	8966348	4.40E-14	4.44E-14
52	1s2 2s1 2p1 (3P) 3d1 4P1.5	8972000	8981681	8972247	4.90E-14	4.94E-14
53	1s2 2s1 2p1 (3P) 3d1 4P0.5	8973000	8985011	8975643	5.65E-14	5.70E-14
54	1s2 2s1 2p1 (3P) 3d1 2F2.5	9030000	9012908	9004790	6.49E-14	6.53E-14
55	1s2 2s1 2p1 (3P) 3d1 2P1.5	9180000	9049954	9043521	6.53E-14	6.56E-14
56	1s2 2s1 2p1 (3P) 3d1 2F3.5	9062000	9066838	9060831	4.45E-14	4.42E-14
59	1s2 2s1 2p1 (3P) 3d1 2P0.5	8967000	9084039	9078984	5.74E-14	5.74E-14
66	1s2 2s1 2p1 (1P) 3d1 2F3.5	9242000	9249517	9250872	7.00E-14	7.18E-14
67	1s2 2s1 2p1 (1P) 3d1 2F2.5	9249000	9251362	9253139	4.85E-14	4.91E-14
69	1s2 2s1 2p1 (1P) 3d1 2D1.5	9134000	9262676	9263777	4.20E-14	4.17E-14
71	1s2 2s1 2p1 (1P) 3d1 2D2.5	9272000	9275516	9276912	4.15E-14	4.14E-14
74	1s2 2s1 2p1 (1P) 3d1 2P1.5	9168000	9299040	9300838	6.00E-14	6.26E-14
126	1s2 2s2 4s1 2S0.5	11050000	11012901	10986106	6.37E-13	5.83E-13
129	1s2 2s2 4d1 2D1.5	11140000	11159006	11135585	1.28E-13	1.24E-13
130	1s2 2s2 4d1 2D2.5	11140000	11162502	11139649	1.28E-13	1.26E-13
142	1s2 2s1 2p1 (3P) 4p1 2P0.5	11465000	11478060	11460571	2.70E-13	2.47E-13
143	1s2 2s1 2p1 (3P) 4p1 2D1.5	11474000	11487446	11470801	2.70E-13	2.64E-13
146	1s2 2s1 2p1 (3P) 4d1 4F2.5	11492000	11509097	11489897	1.78E-13	1.77E-13
149	1s2 2s1 2p1 (3P) 4d1 4D1.5	11526000	11536933	11518812	1.15E-13	1.11E-13
156	1s2 2s1 2p1 (3P) 4d1 2F2.5	11558000	11557332	11541402	1.23E-13	1.18E-13
168	1s2 2s1 2p1 (3P) 4d1 4D3.5	11618000	11618692	11604622	1.26E-13	1.22E-13
169	1s2 2s1 2p1 (3P) 4d1 4D2.5	11618000	11621954	11607936	1.16E-13	1.12E-13
172	1s2 2s1 2p1 (3P) 4d1 2D2.5	11611000	11633161	11620801	1.43E-13	1.38E-13
174	1s2 2s1 2p1 (3P) 4d1 2F3.5	11900000	11652015	11641117	9.77E-14	9.30E-14
194	1s2 2s1 2p1 (1P) 4d1 2F2.5	11897000	11903101	11903215	1.52E-13	1.45E-13
195	1s2 2s1 2p1 (1P) 4d1 2F3.5	11649000	11902966	11903365	2.06E-13	2.01E-13
196	1s2 2s1 2p1 (1P) 4d1 2D2.5	11906000	11908125	11908277	1.06E-13	1.02E-13
270	1s2 2s2 5d1 2D1.5	12359000	12377319	12351697	2.32E-13	2.44E-13

   

Table 4: Comparison of calculated wavelengths ( $\lambda ^{{\rm GRASP}}$, $\lambda ^{{\rm CITRO}}$) and line strengths ( $S^{{\rm GRASP}}$, $S^{{\rm CITRO}}$) for Fe XXII with values presented by NIST ( $\lambda ^{{\rm NIST}}$, $S^{{\rm NIST}}$). Indices of levels in the first two columns are taken from Table 1.

k	i	$\lambda ^{{\rm NIST}}$ (Å)	$\lambda ^{{\rm CITRO}}$ (Å)	$\lambda ^{{\rm GRASP}}$ (Å)	$S^{{\rm NIST}}$	$S^{{\rm CITRO}}$	$S^{{\rm GRASP}}$
1	2	845.52	864.68	847.80	1.33E+00	1.33E+00	1.33E+00
1	3	247.19	250.10	248.20	1.30E-03	1.18E-03	1.24E-03
1	6	135.81	137.18	134.85	5.40E-02	5.29E-02	5.36E-02
1	8	117.14	118.05	116.02	6.20E-02	6.05E-02	6.13E-02
1	9	102.22	103.15	101.39	2.80E-03	2.28E-03	2.32E-03
1	10	100.77	101.70	99.93	1.25E-02	1.25E-02	1.27E-02
1	20	11.77	11.75	11.78	5.10E-02	5.28E-02	5.27E-02
1	126	9.06	9.08	9.10	1.40E-04	2.52E-04	2.10E-004
1	129	8.98	8.96	8.98	6.60E-03	7.61E-03	7.26E-003
2	3	349.30	351.87	350.94	5.90E-04	5.55E-04	5.78E-04
2	4	292.46	295.18	294.05	4.20E-04	3.98E-04	4.16E-04
2	5	253.17	255.61	254.23	3.40E-03	3.30E-03	3.50E-03
2	6	161.74	163.05	160.36	3.20E-04	2.64E-04	2.46E-04
2	7	156.02	157.21	154.85	7.00E-02	6.67E-02	6.75E-02
2	8	136.01	136.71	134.41	3.00E-05	1.65E-04	1.97E-04
2	9	116.26	117.12	115.16	5.48E-02	5.23E-02	5.28E-02
2	10	114.41	115.25	113.28	1.30E-01	1.30E-01	1.32E-01
2	20	11.94	11.91	11.94	1.00E-02	1.06E-02	1.06E-02
2	21	11.92	11.91	11.93	9.00E-02	9.46E-02	9.48E-02
2	126	9.14	9.18	9.20	4.20E-04	5.42E-04	5.02E-04
2	129	9.07	9.06	9.08	1.40E-03	1.54E-03	1.47E-03
2	130	9.07	9.05	9.07	1.20E-02	1.38E-02	1.33E-02
3	11	117.52	118.25	116.65	3.30E-02	3.20E-02	3.24E-02
3	12	100.82	101.54	99.72	6.70E-05	7.28E-05	1.03E-04
3	14	85.83	86.44	84.78	1.40E-04	1.30E-04	1.32E-04
3	42	11.80	11.78	11.80	5.50E-02	5.38E-02	3.32E-02
3	43	11.79	11.78	11.79	4.20E-02	4.31E-02	4.11E-02
3	149	8.99	8.98	9.00	7.00E-03	7.67E-03	7.25E-03
4	11	125.71	126.40	124.67	5.96E-02	5.76E-02	5.81E-02
4	12	106.81	107.49	105.52	5.50E-03	5.10E-03	5.52E-03
4	13	103.45	104.19	102.29	1.60E-04	1.37E-04	1.32E-04
4	15	85.65	86.29	84.66	3.60E-04	3.70E-04	3.97E-04
4	41	11.89	11.87	11.89	6.50E-02	6.87E-02	6.92E-02
4	51	11.75	11.73	11.75	2.30E-02	1.92E-02	1.89E-02
4	52	11.75	11.73	11.75	3.80E-02	3.68E-02	3.68E-02
4	53	11.75	11.72	11.74	2.90E-02	2.78E-02	2.79E-02
4	146	9.07	9.05	9.06	7.70E-03	7.39E-03	7.23E-03
5	11	134.65	135.38	133.53	9.46E-02	9.11E-02	9.27E-02
5	12	113.23	113.91	111.81	6.30E-04	5.83E-04	7.01E-04
5	13	109.53	110.21	108.18	7.40E-03	7.15E-03	7.42E-03
5	15	89.73	90.38	88.66	2.10E-04	1.94E-04	2.04E-04
5	40	11.98	11.96	11.98	4.00E-02	3.97E-02	3.87E-02
5	50	11.84	11.82	11.84	1.50E-01	1.57E-01	1.59E-01
5	51	11.84	11.81	11.83	8.30E-02	8.35E-02	8.37E-02
5	52	11.82	11.80	11.82	2.60E-02	2.64E-02	2.65E-02
5	168	9.01	9.00	9.01	1.60E-02	1.87E-02	1.79E-02
5	169	9.01	9.00	9.01	1.10E-02	1.08E-02	1.01E-02
6	11	192.61	193.58	192.81	1.80E-03	1.81E-03	2.03E-03
6	12	151.54	152.49	150.57	5.20E-02	4.99E-02	5.04E-02
6	13	144.85	145.92	144.06	3.19E-02	2.99E-02	3.03E-02
6	14	120.03	120.80	118.92	5.05E-02	4.73E-02	4.77E-02
6	15	112.21	113.08	111.40	1.40E-02	1.33E-02	1.35E-02
6	49	12.19	12.18	12.21	5.30E-02	4.18E-02	4.02E-02
6	54	12.05	12.07	12.10	3.20E-02	3.55E-02	3.59E-02
6	67	11.75	11.73	11.75	7.70E-02	9.04E-02	9.12E-02
6	156	9.24	9.24	9.26	1.20E-02	1.32E-02	1.23E-02
6	194	8.96	8.95	8.96	8.10E-03	9.98E-03	9.50E-03
7	12	157.03	157.98	155.78	3.80E-02	3.56E-02	3.64E-02
7	13	149.87	150.94	148.82	1.28E-01	1.22E-01	1.23E-01
7	15	115.19	116.07	114.22	4.31E-02	4.09E-02	4.11E-02
7	54	12.10	12.10	12.13	4.10E-02	3.68E-02	3.64E-02
7	56	12.05	12.03	12.05	1.70E-01	1.55E-01	1.53E-01
7	66	11.79	11.77	11.78	7.80E-02	8.88E-02	9.07E-02
7	172	9.22	9.19	9.21	6.30E-03	6.65E-03	6.32E-03
7	174	8.98	9.17	9.19	7.10E-03	2.80E-02	2.62E-02
7	195	9.18	8.97	8.98	2.50E-02	9.27E-03	8.88E-03
8	11	248.62	250.99	251.09	3.60E-03	3.56E-03	3.97E-03
8	12	184.18	186.01	183.90	8.20E-02	7.74E-02	7.83E-02
8	14	139.64	140.92	138.79	7.00E-03	6.93E-03	6.93E-03
8	15	129.17	130.52	128.65	1.59E-02	1.52E-02	1.52E-02
8	55	12.01	12.19	12.22	2.50E-02	2.54E-02	2.53E-02
8	59	12.33	12.14	12.17	2.80E-02	4.60E-03	4.59E-03
8	69	12.08	11.88	11.90	3.50E-02	2.65E-02	2.63E-02
8	74	12.03	11.83	11.85	2.40E-02	3.77E-03	3.80E-03
9	11	360.39	362.21	365.09	1.10E-03	9.46E-04	1.02E-03
9	12	239.12	240.81	238.43	2.30E-02	1.94E-02	1.93E-02
9	14	169.08	170.27	167.74	5.70E-02	5.18E-02	5.25E-02
9	15	153.96	155.32	153.15	1.25E-02	1.26E-02	1.30E-02
9	55	12.19	12.38	12.41	2.60E-02	1.68E-02	1.67E-02
9	59	12.52	12.32	12.36	2.90E-02	2.51E-02	2.49E-02
9	69	12.26	12.06	12.08	3.60E-02	3.34E-02	3.28E-02
10	11	379.64	381.36	385.38	3.30E-03	3.05E-03	3.24E-03
10	12	247.45	249.13	246.92	1.30E-03	1.53E-03	1.56E-03
10	13	230.10	232.06	229.89	1.22E-01	1.15E-01	1.16E-01
10	14	173.21	174.39	171.89	1.10E-02	1.07E-02	1.07E-02
10	15	157.37	158.74	156.61	1.50E-01	1.43E-01	1.45E-01
10	55	12.21	12.40	12.43	3.50E-02	8.48E-03	8.45E-03
10	71	12.08	12.06	12.08	1.30E-01	1.20E-01	1.19E-01
10	196	9.16	9.15	9.17	1.60E-02	1.72E-02	1.64E-02

   

Table 5: The five major spontaneous radiative transition probabilities A^r from each level of Fe XXII and the sum of all radiative probabilities  $\sum A^{r}$ from the corresponding level. Electric dipole, quadrupole and octupole as well as magnetic dipole and quadrupole transitions are included. Arrow marks the final level to which radiative transition happens from the level.

Level	Ar (s-1)	final	Ar (s-1)	final	Ar (s-1)	final	Ar (s-1)	final	Ar (s-1)	final	$\sum A^{r}$ (s-1)
		level		level		level		level		level
2	1.47E+04	$\rightarrow 1$									1.47E+04
3	7.84E+07	$\rightarrow 1$	1.30E+07	$\rightarrow 2$							9.14E+07
4	7.93E+06	$\rightarrow 2$	1.89E+06	$\rightarrow 1$	3.60E+03	$\rightarrow 3$					9.82E+06
5	6.78E+07	$\rightarrow 2$	2.36E+03	$\rightarrow 4$	6.81E+00	$\rightarrow 1$	6.27E-01	$\rightarrow 3$			6.78E+07
6	1.09E+10	$\rightarrow 1$	3.25E+07	$\rightarrow 2$	7.86E+03	$\rightarrow 4$	4.95E+03	$\rightarrow 5$	3.50E+03	$\rightarrow 3$	1.10E+10
7	6.06E+09	$\rightarrow 2$	3.10E+04	$\rightarrow 5$	1.42E+04	$\rightarrow 4$	1.10E+02	$\rightarrow 6$	3.93E+01	$\rightarrow 1$	6.06E+09
8	3.92E+10	$\rightarrow 1$	6.88E+07	$\rightarrow 2$	5.52E+04	$\rightarrow 4$	5.48E+04	$\rightarrow 3$	7.23E+02	$\rightarrow 6$	3.93E+10
9	3.47E+10	$\rightarrow 2$	2.22E+09	$\rightarrow 1$	1.01E+05	$\rightarrow 4$	1.69E+04	$\rightarrow 8$	5.53E+03	$\rightarrow 6$	3.69E+10
10	4.52E+10	$\rightarrow 2$	6.36E+09	$\rightarrow 1$	2.01E+04	$\rightarrow 6$	1.67E+04	$\rightarrow 4$	1.43E+04	$\rightarrow 8$	5.16E+10
11	1.94E+10	$\rightarrow 5$	1.51E+10	$\rightarrow 4$	1.02E+10	$\rightarrow 3$	1.28E+08	$\rightarrow 6$	1.14E+08	$\rightarrow 8$	4.49E+10
12	7.41E+09	$\rightarrow 6$	6.30E+09	$\rightarrow 8$	4.77E+09	$\rightarrow 7$	2.20E+09	$\rightarrow 4$	7.26E+08	$\rightarrow 9$	2.17E+10
13	1.25E+10	$\rightarrow 7$	3.38E+09	$\rightarrow 6$	3.18E+09	$\rightarrow 10$	1.91E+09	$\rightarrow 5$	4.34E+07	$\rightarrow 4$	2.10E+10
14	2.85E+10	$\rightarrow 6$	1.11E+10	$\rightarrow 9$	2.62E+09	$\rightarrow 8$	2.13E+09	$\rightarrow 10$	2.17E+08	$\rightarrow 3$	4.46E+10
15	1.89E+10	$\rightarrow 10$	1.39E+10	$\rightarrow 7$	4.87E+09	$\rightarrow 6$	3.62E+09	$\rightarrow 8$	1.78E+09	$\rightarrow 9$	4.35E+10
16	1.90E+12	$\rightarrow 2$	8.94E+11	$\rightarrow 1$	1.18E+08	$\rightarrow 15$	9.19E+07	$\rightarrow 11$	5.64E+07	$\rightarrow 12$	2.79E+12
17	1.92E+11	$\rightarrow 6$	3.71E+10	$\rightarrow 9$	3.90E+09	$\rightarrow 2$	3.74E+09	$\rightarrow 4$	1.00E+09	$\rightarrow 16$	2.38E+11
18	1.56E+11	$\rightarrow 7$	2.70E+10	$\rightarrow 8$	2.56E+10	$\rightarrow 10$	2.30E+10	$\rightarrow 5$	1.06E+10	$\rightarrow 6$	2.52E+11
19	2.48E+12	$\rightarrow 4$	5.38E+11	$\rightarrow 3$	2.84E+10	$\rightarrow 6$	3.85E+09	$\rightarrow 9$	6.30E+08	$\rightarrow 8$	3.05E+12
20	1.64E+13	$\rightarrow 1$	3.15E+12	$\rightarrow 2$	1.21E+09	$\rightarrow 12$	8.63E+08	$\rightarrow 17$	1.13E+08	$\rightarrow 8$	1.95E+13
21	1.88E+13	$\rightarrow 2$	1.10E+09	$\rightarrow 13$	7.29E+08	$\rightarrow 18$	2.19E+08	$\rightarrow 15$	1.38E+08	$\rightarrow 11$	1.88E+13
22	1.45E+12	$\rightarrow 5$	1.33E+12	$\rightarrow 3$	3.47E+11	$\rightarrow 4$	3.52E+10	$\rightarrow 6$	2.41E+10	$\rightarrow 7$	3.19E+12
23	1.54E+12	$\rightarrow 6$	6.16E+11	$\rightarrow 8$	5.13E+10	$\rightarrow 9$	2.54E+10	$\rightarrow 4$	4.83E+09	$\rightarrow 10$	2.24E+12
24	2.20E+12	$\rightarrow 5$	1.12E+12	$\rightarrow 4$	1.06E+11	$\rightarrow 7$	3.01E+09	$\rightarrow 6$	2.66E+09	$\rightarrow 10$	3.42E+12
25	1.53E+12	$\rightarrow 1$	2.18E+11	$\rightarrow 2$	1.46E+10	$\rightarrow 12$	2.95E+09	$\rightarrow 4$	2.25E+09	$\rightarrow 14$	1.77E+12
26	7.38E+11	$\rightarrow 2$	7.17E+11	$\rightarrow 1$	1.01E+10	$\rightarrow 13$	2.06E+09	$\rightarrow 14$	1.22E+09	$\rightarrow 4$	1.47E+12
27	1.89E+12	$\rightarrow 7$	5.21E+11	$\rightarrow 9$	2.05E+11	$\rightarrow 8$	1.47E+11	$\rightarrow 6$	1.23E+11	$\rightarrow 10$	2.94E+12
28	2.35E+12	$\rightarrow 1$	9.90E+11	$\rightarrow 2$	3.09E+10	$\rightarrow 13$	3.44E+09	$\rightarrow 11$	3.26E+09	$\rightarrow 14$	3.38E+12
29	6.49E+12	$\rightarrow 1$	6.12E+11	$\rightarrow 2$	1.16E+11	$\rightarrow 12$	5.06E+09	$\rightarrow 11$	5.03E+09	$\rightarrow 14$	7.23E+12
30	4.15E+10	$\rightarrow 2$	2.93E+09	$\rightarrow 11$	2.02E+09	$\rightarrow 3$	1.64E+09	$\rightarrow 5$	1.48E+09	$\rightarrow 22$	5.09E+10
31	2.52E+11	$\rightarrow 1$	1.52E+11	$\rightarrow 2$	2.53E+10	$\rightarrow 11$	3.31E+09	$\rightarrow 14$	2.91E+09	$\rightarrow 15$	4.42E+11
32	4.91E+12	$\rightarrow 1$	5.06E+10	$\rightarrow 2$	3.85E+10	$\rightarrow 13$	1.21E+10	$\rightarrow 12$	8.63E+09	$\rightarrow 14$	5.03E+12
33	2.27E+09	$\rightarrow 5$	1.62E+09	$\rightarrow 4$	1.43E+09	$\rightarrow 24$	1.18E+08	$\rightarrow 7$	1.73E+07	$\rightarrow 13$	5.47E+09
34	3.26E+12	$\rightarrow 2$	1.04E+12	$\rightarrow 1$	4.01E+10	$\rightarrow 12$	7.58E+09	$\rightarrow 13$	7.20E+09	$\rightarrow 14$	4.36E+12
35	6.48E+11	$\rightarrow 4$	6.38E+11	$\rightarrow 3$	4.97E+11	$\rightarrow 6$	4.72E+10	$\rightarrow 5$	2.27E+10	$\rightarrow 7$	1.87E+12
36	2.56E+12	$\rightarrow 2$	7.38E+11	$\rightarrow 1$	2.19E+10	$\rightarrow 12$	1.23E+10	$\rightarrow 11$	6.51E+09	$\rightarrow 13$	3.35E+12
37	2.13E+12	$\rightarrow 2$	1.43E+10	$\rightarrow 13$	1.22E+10	$\rightarrow 11$	9.91E+09	$\rightarrow 15$	1.61E+09	$\rightarrow 24$	2.17E+12
38	2.78E+12	$\rightarrow 4$	7.49E+11	$\rightarrow 5$	1.76E+11	$\rightarrow 7$	1.03E+11	$\rightarrow 6$	1.46E+09	$\rightarrow 10$	3.81E+12
39	7.32E+12	$\rightarrow 2$	6.68E+10	$\rightarrow 13$	2.08E+10	$\rightarrow 15$	1.32E+10	$\rightarrow 11$	1.09E+09	$\rightarrow 18$	7.43E+12
40	5.84E+12	$\rightarrow 5$	2.49E+11	$\rightarrow 7$	4.96E+08	$\rightarrow 30$	2.91E+07	$\rightarrow 2$	7.05E+06	$\rightarrow 21$	6.09E+12
41	1.38E+13	$\rightarrow 4$	1.23E+12	$\rightarrow 7$	1.13E+12	$\rightarrow 5$	5.26E+11	$\rightarrow 6$	1.68E+11	$\rightarrow 10$	1.69E+13
42	1.66E+13	$\rightarrow 3$	5.23E+12	$\rightarrow 4$	1.11E+12	$\rightarrow 6$	2.93E+11	$\rightarrow 8$	2.27E+11	$\rightarrow 5$	2.36E+13
43	2.66E+13	$\rightarrow 3$	1.27E+12	$\rightarrow 4$	2.62E+11	$\rightarrow 6$	2.12E+11	$\rightarrow 9$	5.16E+10	$\rightarrow 10$	2.84E+13
44	7.66E+12	$\rightarrow 2$	1.53E+12	$\rightarrow 1$	1.82E+11	$\rightarrow 15$	9.42E+10	$\rightarrow 14$	2.07E+10	$\rightarrow 11$	9.51E+12
45	1.71E+12	$\rightarrow 9$	1.23E+12	$\rightarrow 6$	9.69E+11	$\rightarrow 10$	9.34E+11	$\rightarrow 3$	4.22E+10	$\rightarrow 8$	4.92E+12
46	2.25E+12	$\rightarrow 8$	1.15E+12	$\rightarrow 10$	9.86E+11	$\rightarrow 6$	7.98E+11	$\rightarrow 7$	5.62E+11	$\rightarrow 3$	6.08E+12
47	3.74E+12	$\rightarrow 6$	3.21E+12	$\rightarrow 8$	1.28E+12	$\rightarrow 3$	5.75E+11	$\rightarrow 10$	5.64E+11	$\rightarrow 7$	1.02E+13
48	4.56E+08	$\rightarrow 33$	1.24E+07	$\rightarrow 7$	1.67E+06	$\rightarrow 5$	9.33E+05	$\rightarrow 4$	7.28E+03	$\rightarrow 24$	4.70E+08
49	7.75E+12	$\rightarrow 6$	4.71E+12	$\rightarrow 4$	1.23E+12	$\rightarrow 7$	6.54E+11	$\rightarrow 10$	2.64E+11	$\rightarrow 5$	1.46E+13
50	2.40E+13	$\rightarrow 5$	2.21E+11	$\rightarrow 7$	2.59E+08	$\rightarrow 37$	2.34E+08	$\rightarrow 33$	7.73E+07	$\rightarrow 2$	2.42E+13
51	1.70E+13	$\rightarrow 5$	4.00E+12	$\rightarrow 4$	1.17E+12	$\rightarrow 6$	3.20E+11	$\rightarrow 7$	1.44E+10	$\rightarrow 10$	2.25E+13
52	1.15E+13	$\rightarrow 4$	8.10E+12	$\rightarrow 5$	3.09E+11	$\rightarrow 7$	1.49E+11	$\rightarrow 8$	1.11E+11	$\rightarrow 3$	2.03E+13
53	1.74E+13	$\rightarrow 4$	5.08E+10	$\rightarrow 3$	3.72E+10	$\rightarrow 10$	3.19E+10	$\rightarrow 6$	1.57E+10	$\rightarrow 9$	1.75E+13
54	6.96E+12	$\rightarrow 7$	6.76E+12	$\rightarrow 6$	1.02E+12	$\rightarrow 10$	4.20E+11	$\rightarrow 5$	1.32E+11	$\rightarrow 4$	1.53E+13
55	7.05E+12	$\rightarrow 8$	4.44E+12	$\rightarrow 9$	2.24E+12	$\rightarrow 10$	9.64E+11	$\rightarrow 7$	3.20E+11	$\rightarrow 6$	1.53E+13
56	2.25E+13	$\rightarrow 7$	1.23E+11	$\rightarrow 5$	1.50E+10	$\rightarrow 2$	1.10E+09	$\rightarrow 39$	4.12E+08	$\rightarrow 37$	2.26E+13
57	1.99E+12	$\rightarrow 2$	7.91E+11	$\rightarrow 1$	5.31E+11	$\rightarrow 12$	1.46E+11	$\rightarrow 14$	7.69E+10	$\rightarrow 11$	3.56E+12
58	1.74E+12	$\rightarrow 2$	1.44E+11	$\rightarrow 13$	2.13E+10	$\rightarrow 14$	1.82E+10	$\rightarrow 15$	1.78E+10	$\rightarrow 17$	1.97E+12
59	1.35E+13	$\rightarrow 9$	2.59E+12	$\rightarrow 8$	9.03E+11	$\rightarrow 10$	2.79E+11	$\rightarrow 6$	1.56E+11	$\rightarrow 3$	1.74E+13
60	1.08E+12	$\rightarrow 2$	1.63E+10	$\rightarrow 18$	7.82E+09	$\rightarrow 15$	6.10E+09	$\rightarrow 12$	1.91E+09	$\rightarrow 11$	1.12E+12
61	1.53E+12	$\rightarrow 2$	4.55E+11	$\rightarrow 1$	3.78E+11	$\rightarrow 13$	1.20E+11	$\rightarrow 15$	3.04E+10	$\rightarrow 14$	2.57E+12
62	9.67E+11	$\rightarrow 11$	2.75E+11	$\rightarrow 2$	5.93E+10	$\rightarrow 12$	1.40E+10	$\rightarrow 14$	1.22E+10	$\rightarrow 1$	1.35E+12
63	6.34E+11	$\rightarrow 11$	4.71E+11	$\rightarrow 1$	1.26E+11	$\rightarrow 2$	1.97E+10	$\rightarrow 14$	1.86E+10	$\rightarrow 12$	1.30E+12
64	1.53E+12	$\rightarrow 11$	1.34E+11	$\rightarrow 12$	9.37E+10	$\rightarrow 2$	1.10E+10	$\rightarrow 13$	8.82E+09	$\rightarrow 19$	1.79E+12
65	1.74E+12	$\rightarrow 11$	3.24E+11	$\rightarrow 13$	8.22E+10	$\rightarrow 2$	9.14E+09	$\rightarrow 24$	6.66E+09	$\rightarrow 22$	2.17E+12
66	1.38E+13	$\rightarrow 7$	1.55E+11	$\rightarrow 5$	1.20E+10	$\rightarrow 21$	4.43E+09	$\rightarrow 2$	5.04E+08	$\rightarrow 60$	1.39E+13
67	1.88E+13	$\rightarrow 6$	1.47E+12	$\rightarrow 7$	2.42E+10	$\rightarrow 5$	2.39E+10	$\rightarrow 10$	2.08E+10	$\rightarrow 4$	2.04E+13
68	2.41E+12	$\rightarrow 12$	7.73E+11	$\rightarrow 14$	4.86E+11	$\rightarrow 1$	2.86E+11	$\rightarrow 2$	1.01E+11	$\rightarrow 15$	4.09E+12
69	9.60E+12	$\rightarrow 9$	7.97E+12	$\rightarrow 8$	3.18E+12	$\rightarrow 6$	3.08E+12	$\rightarrow 10$	1.12E+11	$\rightarrow 7$	2.40E+13
70	4.32E+12	$\rightarrow 8$	2.10E+12	$\rightarrow 3$	3.33E+11	$\rightarrow 9$	5.44E+10	$\rightarrow 10$	8.75E+09	$\rightarrow 26$	6.84E+12
71	2.30E+13	$\rightarrow 10$	7.97E+11	$\rightarrow 7$	3.75E+11	$\rightarrow 6$	2.21E+10	$\rightarrow 21$	9.27E+09	$\rightarrow 4$	2.42E+13
72	1.64E+12	$\rightarrow 13$	8.41E+11	$\rightarrow 14$	5.95E+11	$\rightarrow 12$	3.29E+11	$\rightarrow 2$	2.06E+11	$\rightarrow 1$	3.81E+12
73	1.02E+13	$\rightarrow 8$	3.36E+12	$\rightarrow 10$	1.05E+12	$\rightarrow 6$	3.94E+11	$\rightarrow 3$	4.88E+10	$\rightarrow 9$	1.51E+13
74	8.15E+12	$\rightarrow 10$	5.78E+12	$\rightarrow 9$	1.15E+12	$\rightarrow 8$	4.84E+11	$\rightarrow 3$	2.59E+11	$\rightarrow 7$	1.60E+13
75	2.45E+12	$\rightarrow 3$	1.75E+12	$\rightarrow 9$	8.69E+11	$\rightarrow 10$	4.60E+11	$\rightarrow 4$	7.62E+10	$\rightarrow 7$	5.65E+12
76	1.66E+12	$\rightarrow 4$	1.48E+12	$\rightarrow 10$	5.64E+11	$\rightarrow 8$	4.36E+11	$\rightarrow 9$	2.76E+11	$\rightarrow 3$	4.70E+12
77	1.59E+12	$\rightarrow 4$	9.11E+11	$\rightarrow 8$	7.68E+11	$\rightarrow 9$	6.06E+11	$\rightarrow 5$	2.51E+11	$\rightarrow 3$	4.46E+12
78	3.15E+12	$\rightarrow 4$	2.36E+11	$\rightarrow 5$	3.43E+10	$\rightarrow 10$	4.35E+09	$\rightarrow 30$	3.63E+09	$\rightarrow 33$	3.45E+12
79	2.13E+12	$\rightarrow 4$	1.11E+12	$\rightarrow 8$	5.37E+11	$\rightarrow 9$	4.87E+11	$\rightarrow 3$	2.99E+11	$\rightarrow 6$	4.81E+12
80	1.92E+12	$\rightarrow 13$	7.00E+11	$\rightarrow 12$	4.97E+11	$\rightarrow 15$	1.31E+11	$\rightarrow 11$	1.24E+11	$\rightarrow 2$	3.38E+12
81	2.30E+12	$\rightarrow 5$	1.13E+12	$\rightarrow 10$	3.82E+11	$\rightarrow 7$	3.67E+11	$\rightarrow 4$	9.47E+10	$\rightarrow 6$	4.29E+12
82	1.32E+12	$\rightarrow 8$	1.01E+12	$\rightarrow 6$	7.22E+11	$\rightarrow 4$	6.55E+11	$\rightarrow 10$	5.18E+11	$\rightarrow 9$	5.00E+12
83	2.19E+12	$\rightarrow 15$	8.41E+11	$\rightarrow 12$	2.99E+11	$\rightarrow 13$	2.67E+11	$\rightarrow 2$	8.05E+10	$\rightarrow 14$	3.73E+12
84	3.27E+12	$\rightarrow 5$	4.48E+10	$\rightarrow 7$	8.68E+09	$\rightarrow 33$	4.83E+09	$\rightarrow 30$	1.95E+09	$\rightarrow 11$	3.33E+12
85	6.02E+11	$\rightarrow 11$	6.00E+11	$\rightarrow 12$	7.46E+10	$\rightarrow 15$	6.46E+10	$\rightarrow 1$	3.67E+10	$\rightarrow 14$	1.41E+12
86	2.18E+12	$\rightarrow 5$	1.16E+12	$\rightarrow 4$	7.37E+11	$\rightarrow 7$	6.08E+11	$\rightarrow 10$	4.56E+11	$\rightarrow 6$	5.66E+12
87	2.14E+12	$\rightarrow 11$	5.77E+11	$\rightarrow 12$	1.20E+11	$\rightarrow 13$	8.94E+09	$\rightarrow 2$	8.16E+09	$\rightarrow 3$	2.87E+12
88	1.77E+12	$\rightarrow 10$	1.37E+12	$\rightarrow 5$	1.09E+12	$\rightarrow 6$	2.41E+11	$\rightarrow 7$	7.56E+10	$\rightarrow 4$	4.56E+12
89	1.74E+12	$\rightarrow 5$	1.28E+12	$\rightarrow 8$	1.27E+12	$\rightarrow 10$	1.12E+12	$\rightarrow 6$	4.85E+11	$\rightarrow 9$	6.35E+12
90	3.97E+12	$\rightarrow 10$	8.66E+11	$\rightarrow 8$	3.20E+11	$\rightarrow 9$	9.86E+10	$\rightarrow 4$	3.87E+10	$\rightarrow 3$	5.33E+12
91	3.35E+11	$\rightarrow 13$	9.88E+09	$\rightarrow 4$	3.95E+09	$\rightarrow 48$	3.37E+09	$\rightarrow 40$	2.47E+09	$\rightarrow 38$	3.59E+11
92	2.16E+12	$\rightarrow 11$	8.39E+11	$\rightarrow 13$	7.54E+11	$\rightarrow 15$	5.22E+11	$\rightarrow 14$	4.76E+11	$\rightarrow 12$	4.83E+12
93	2.63E+12	$\rightarrow 11$	3.58E+11	$\rightarrow 12$	1.93E+10	$\rightarrow 13$	8.96E+09	$\rightarrow 15$	4.34E+09	$\rightarrow 4$	3.03E+12
94	6.83E+11	$\rightarrow 11$	5.84E+11	$\rightarrow 14$	3.25E+11	$\rightarrow 12$	1.88E+11	$\rightarrow 15$	1.46E+10	$\rightarrow 35$	1.82E+12
95	1.61E+12	$\rightarrow 6$	1.43E+12	$\rightarrow 10$	5.52E+11	$\rightarrow 7$	1.06E+11	$\rightarrow 5$	5.27E+10	$\rightarrow 4$	3.76E+12
96	6.88E+09	$\rightarrow 5$	2.61E+09	$\rightarrow 41$	2.23E+09	$\rightarrow 48$	1.72E+09	$\rightarrow 50$	1.59E+09	$\rightarrow 40$	2.14E+10
97	1.03E+10	$\rightarrow 5$	7.30E+09	$\rightarrow 48$	3.01E+09	$\rightarrow 40$	6.60E+08	$\rightarrow 50$	4.63E+08	$\rightarrow 84$	2.21E+10
98	4.31E+12	$\rightarrow 12$	7.46E+11	$\rightarrow 11$	6.24E+11	$\rightarrow 15$	5.02E+11	$\rightarrow 14$	2.17E+11	$\rightarrow 13$	6.46E+12
99	6.31E+12	$\rightarrow 11$	2.31E+12	$\rightarrow 12$	7.81E+11	$\rightarrow 13$	4.82E+10	$\rightarrow 15$	4.12E+09	$\rightarrow 40$	9.47E+12
100	3.19E+12	$\rightarrow 7$	1.52E+11	$\rightarrow 5$	4.76E+09	$\rightarrow 60$	3.58E+09	$\rightarrow 33$	1.48E+09	$\rightarrow 13$	3.36E+12
101	2.96E+12	$\rightarrow 7$	1.18E+12	$\rightarrow 8$	1.18E+12	$\rightarrow 6$	6.26E+11	$\rightarrow 10$	2.79E+11	$\rightarrow 9$	6.43E+12
102	3.76E+12	$\rightarrow 7$	3.12E+12	$\rightarrow 10$	1.12E+11	$\rightarrow 6$	3.23E+09	$\rightarrow 37$	2.90E+09	$\rightarrow 58$	7.01E+12
103	1.69E+13	$\rightarrow 11$	2.37E+12	$\rightarrow 13$	1.12E+11	$\rightarrow 15$	2.53E+10	$\rightarrow 12$	1.81E+10	$\rightarrow 2$	1.94E+13
104	5.87E+12	$\rightarrow 14$	2.21E+12	$\rightarrow 11$	2.71E+11	$\rightarrow 15$	8.64E+10	$\rightarrow 12$	7.14E+10	$\rightarrow 1$	8.60E+12
105	4.31E+12	$\rightarrow 6$	2.38E+11	$\rightarrow 10$	1.49E+11	$\rightarrow 8$	1.39E+11	$\rightarrow 9$	4.08E+09	$\rightarrow 4$	4.86E+12
106	2.42E+13	$\rightarrow 11$	9.87E+11	$\rightarrow 13$	4.01E+10	$\rightarrow 14$	3.69E+10	$\rightarrow 2$	8.46E+09	$\rightarrow 5$	2.53E+13
107	3.81E+12	$\rightarrow 15$	2.27E+12	$\rightarrow 14$	1.64E+12	$\rightarrow 11$	6.20E+10	$\rightarrow 2$	3.76E+10	$\rightarrow 1$	7.85E+12
108	2.32E+13	$\rightarrow 11$	1.79E+12	$\rightarrow 14$	1.35E+11	$\rightarrow 15$	4.52E+10	$\rightarrow 2$	4.22E+10	$\rightarrow 12$	2.53E+13
109	7.20E+12	$\rightarrow 13$	3.15E+09	$\rightarrow 6$	2.48E+09	$\rightarrow 5$	2.47E+09	$\rightarrow 49$	2.43E+09	$\rightarrow 56$	7.22E+12
110	2.00E+13	$\rightarrow 12$	5.56E+12	$\rightarrow 13$	9.88E+11	$\rightarrow 11$	5.10E+11	$\rightarrow 15$	1.58E+11	$\rightarrow 2$	2.73E+13
111	1.32E+13	$\rightarrow 14$	1.26E+12	$\rightarrow 15$	1.09E+12	$\rightarrow 13$	3.44E+11	$\rightarrow 1$	7.78E+10	$\rightarrow 11$	1.60E+13
112	2.99E+12	$\rightarrow 10$	1.25E+12	$\rightarrow 7$	9.25E+11	$\rightarrow 6$	3.01E+10	$\rightarrow 5$	2.34E+10	$\rightarrow 4$	5.24E+12
113	2.18E+12	$\rightarrow 13$	6.25E+09	$\rightarrow 6$	1.76E+09	$\rightarrow 7$	1.54E+09	$\rightarrow 10$	1.45E+09	$\rightarrow 48$	2.19E+12
114	9.69E+09	$\rightarrow 7$	2.95E+09	$\rightarrow 48$	2.02E+09	$\rightarrow 66$	5.73E+08	$\rightarrow 100$	4.20E+08	$\rightarrow 5$	1.60E+10
115	1.39E+13	$\rightarrow 12$	3.52E+12	$\rightarrow 13$	1.91E+12	$\rightarrow 14$	3.48E+11	$\rightarrow 11$	1.84E+11	$\rightarrow 15$	1.99E+13
116	1.25E+13	$\rightarrow 13$	1.08E+13	$\rightarrow 12$	1.57E+12	$\rightarrow 15$	3.63E+11	$\rightarrow 11$	2.72E+10	$\rightarrow 2$	2.53E+13
117	3.29E+13	$\rightarrow 13$	5.22E+09	$\rightarrow 7$	4.33E+09	$\rightarrow 56$	3.62E+09	$\rightarrow 10$	1.63E+09	$\rightarrow 67$	3.29E+13
118	8.35E+12	$\rightarrow 12$	8.03E+12	$\rightarrow 14$	1.57E+11	$\rightarrow 15$	1.04E+11	$\rightarrow 1$	7.73E+10	$\rightarrow 11$	1.68E+13
119	4.76E+12	$\rightarrow 9$	3.47E+11	$\rightarrow 8$	2.25E+11	$\rightarrow 10$	2.88E+10	$\rightarrow 6$	2.41E+10	$\rightarrow 58$	5.40E+12
120	1.98E+13	$\rightarrow 15$	5.67E+12	$\rightarrow 12$	7.54E+11	$\rightarrow 13$	2.12E+11	$\rightarrow 2$	1.11E+11	$\rightarrow 11$	2.66E+13
121	9.83E+12	$\rightarrow 15$	2.75E+12	$\rightarrow 12$	1.11E+12	$\rightarrow 14$	4.71E+11	$\rightarrow 11$	1.35E+11	$\rightarrow 2$	1.43E+13
122	1.83E+13	$\rightarrow 15$	1.89E+12	$\rightarrow 13$	1.19E+12	$\rightarrow 14$	3.21E+11	$\rightarrow 11$	2.27E+11	$\rightarrow 2$	2.20E+13
123	2.92E+12	$\rightarrow 9$	1.22E+12	$\rightarrow 8$	4.84E+11	$\rightarrow 10$	1.89E+10	$\rightarrow 60$	1.02E+10	$\rightarrow 61$	4.67E+12
124	1.34E+13	$\rightarrow 15$	4.98E+11	$\rightarrow 13$	1.44E+11	$\rightarrow 12$	4.88E+10	$\rightarrow 2$	2.93E+10	$\rightarrow 11$	1.41E+13
125	1.55E+13	$\rightarrow 14$	3.48E+12	$\rightarrow 15$	1.15E+11	$\rightarrow 12$	6.98E+10	$\rightarrow 13$	1.96E+10	$\rightarrow 67$	1.92E+13
126	7.05E+11	$\rightarrow 2$	4.39E+11	$\rightarrow 18$	3.39E+11	$\rightarrow 1$	2.09E+11	$\rightarrow 17$	1.09E+10	$\rightarrow 27$	1.71E+12
127	7.15E+11	$\rightarrow 16$	1.32E+11	$\rightarrow 20$	4.43E+10	$\rightarrow 9$	3.89E+10	$\rightarrow 8$	1.25E+10	$\rightarrow 6$	9.58E+11
128	6.85E+11	$\rightarrow 16$	1.13E+11	$\rightarrow 21$	4.62E+10	$\rightarrow 9$	3.85E+10	$\rightarrow 8$	1.24E+10	$\rightarrow 20$	9.22E+11
129	5.32E+12	$\rightarrow 1$	1.36E+12	$\rightarrow 17$	1.04E+12	$\rightarrow 2$	2.73E+11	$\rightarrow 18$	4.26E+10	$\rightarrow 23$	8.06E+12
130	6.25E+12	$\rightarrow 2$	1.63E+12	$\rightarrow 18$	4.47E+10	$\rightarrow 27$	1.48E+10	$\rightarrow 22$	4.59E+09	$\rightarrow 74$	7.95E+12
131	3.17E+12	$\rightarrow 20$	2.26E+11	$\rightarrow 21$	1.07E+10	$\rightarrow 58$	5.51E+09	$\rightarrow 1$	3.89E+09	$\rightarrow 61$	3.43E+12
132	3.39E+12	$\rightarrow 21$	1.44E+10	$\rightarrow 60$	7.13E+09	$\rightarrow 2$	2.70E+09	$\rightarrow 7$	2.26E+09	$\rightarrow 30$	3.42E+12
133	6.96E+11	$\rightarrow 4$	3.23E+11	$\rightarrow 28$	1.72E+11	$\rightarrow 25$	1.70E+11	$\rightarrow 3$	8.33E+10	$\rightarrow 6$	1.65E+12
134	4.57E+11	$\rightarrow 5$	4.13E+11	$\rightarrow 3$	2.93E+11	$\rightarrow 30$	1.28E+11	$\rightarrow 31$	1.16E+11	$\rightarrow 26$	1.74E+12
135	6.99E+11	$\rightarrow 6$	2.96E+11	$\rightarrow 8$	2.65E+11	$\rightarrow 32$	1.88E+11	$\rightarrow 29$	7.54E+10	$\rightarrow 26$	1.74E+12
136	7.83E+11	$\rightarrow 1$	6.08E+11	$\rightarrow 19$	1.06E+11	$\rightarrow 35$	7.13E+10	$\rightarrow 23$	4.50E+10	$\rightarrow 2$	1.71E+12
137	5.90E+11	$\rightarrow 19$	1.19E+11	$\rightarrow 1$	1.07E+11	$\rightarrow 22$	8.46E+10	$\rightarrow 38$	2.90E+10	$\rightarrow 2$	9.85E+11
138	1.52E+12	$\rightarrow 1$	3.94E+11	$\rightarrow 22$	3.68E+11	$\rightarrow 2$	2.15E+11	$\rightarrow 23$	7.39E+10	$\rightarrow 41$	2.78E+12
139	7.44E+11	$\rightarrow 5$	6.41E+11	$\rightarrow 4$	2.76E+11	$\rightarrow 33$	2.06E+11	$\rightarrow 37$	8.14E+10	$\rightarrow 36$	2.13E+12
140	5.06E+11	$\rightarrow 22$	4.38E+11	$\rightarrow 1$	2.74E+11	$\rightarrow 2$	8.66E+10	$\rightarrow 23$	8.25E+10	$\rightarrow 19$	1.54E+12
141	6.80E+11	$\rightarrow 22$	1.83E+11	$\rightarrow 2$	8.84E+10	$\rightarrow 40$	1.33E+10	$\rightarrow 41$	7.75E+09	$\rightarrow 38$	1.01E+12
142	3.15E+12	$\rightarrow 1$	4.88E+11	$\rightarrow 23$	1.48E+11	$\rightarrow 22$	9.43E+10	$\rightarrow 47$	4.66E+10	$\rightarrow 14$	4.05E+12
143	2.88E+12	$\rightarrow 1$	4.55E+11	$\rightarrow 23$	1.61E+11	$\rightarrow 22$	7.92E+10	$\rightarrow 49$	4.99E+10	$\rightarrow 14$	3.79E+12
144	1.30E+12	$\rightarrow 25$	7.17E+11	$\rightarrow 3$	4.57E+11	$\rightarrow 4$	2.25E+11	$\rightarrow 6$	1.62E+11	$\rightarrow 26$	3.26E+12
145	7.70E+11	$\rightarrow 7$	2.66E+11	$\rightarrow 39$	2.14E+11	$\rightarrow 9$	1.11E+11	$\rightarrow 10$	1.10E+11	$\rightarrow 44$	1.93E+12
146	3.35E+12	$\rightarrow 4$	9.28E+11	$\rightarrow 28$	6.56E+11	$\rightarrow 26$	5.05E+11	$\rightarrow 6$	1.05E+11	$\rightarrow 5$	5.66E+12
147	1.64E+12	$\rightarrow 4$	7.42E+11	$\rightarrow 5$	6.54E+11	$\rightarrow 26$	4.98E+11	$\rightarrow 28$	3.75E+11	$\rightarrow 30$	4.85E+12
148	3.52E+12	$\rightarrow 5$	1.57E+12	$\rightarrow 30$	4.14E+11	$\rightarrow 7$	1.26E+11	$\rightarrow 37$	4.51E+09	$\rightarrow 33$	5.65E+12
149	5.34E+12	$\rightarrow 3$	1.31E+12	$\rightarrow 4$	6.73E+11	$\rightarrow 31$	3.89E+11	$\rightarrow 26$	3.47E+11	$\rightarrow 32$	8.99E+12
150	8.88E+12	$\rightarrow 3$	1.23E+12	$\rightarrow 31$	2.93E+11	$\rightarrow 4$	1.72E+11	$\rightarrow 25$	1.69E+11	$\rightarrow 26$	1.11E+13
151	2.50E+12	$\rightarrow 35$	3.25E+11	$\rightarrow 47$	2.20E+11	$\rightarrow 42$	9.67E+10	$\rightarrow 41$	9.38E+10	$\rightarrow 38$	3.42E+12
152	1.54E+12	$\rightarrow 41$	1.46E+12	$\rightarrow 38$	1.55E+11	$\rightarrow 54$	1.24E+11	$\rightarrow 49$	6.50E+10	$\rightarrow 51$	3.37E+12
153	3.54E+12	$\rightarrow 8$	1.16E+12	$\rightarrow 29$	1.13E+12	$\rightarrow 6$	1.72E+11	$\rightarrow 3$	1.10E+11	$\rightarrow 26$	6.52E+12
154	1.24E+12	$\rightarrow 2$	4.29E+11	$\rightarrow 24$	2.58E+11	$\rightarrow 27$	3.64E+10	$\rightarrow 51$	2.82E+10	$\rightarrow 52$	2.14E+12
155	6.96E+11	$\rightarrow 24$	8.42E+10	$\rightarrow 48$	2.30E+10	$\rightarrow 50$	1.93E+10	$\rightarrow 51$	4.38E+09	$\rightarrow 41$	8.38E+11
156	5.59E+12	$\rightarrow 6$	1.34E+12	$\rightarrow 32$	1.04E+12	$\rightarrow 4$	8.66E+10	$\rightarrow 5$	8.21E+10	$\rightarrow 10$	8.46E+12
157	7.57E+11	$\rightarrow 2$	5.69E+11	$\rightarrow 24$	1.32E+11	$\rightarrow 27$	5.47E+10	$\rightarrow 50$	2.16E+10	$\rightarrow 51$	1.63E+12
158	1.86E+12	$\rightarrow 2$	3.73E+11	$\rightarrow 27$	2.49E+11	$\rightarrow 24$	8.54E+10	$\rightarrow 43$	5.81E+10	$\rightarrow 54$	2.87E+12
159	2.13E+12	$\rightarrow 43$	7.13E+11	$\rightarrow 42$	1.56E+11	$\rightarrow 35$	1.12E+11	$\rightarrow 2$	6.20E+10	$\rightarrow 45$	3.43E+12
160	1.66E+12	$\rightarrow 38$	8.21E+11	$\rightarrow 41$	5.57E+11	$\rightarrow 49$	2.22E+11	$\rightarrow 40$	7.26E+10	$\rightarrow 54$	3.41E+12
161	2.37E+12	$\rightarrow 42$	3.53E+11	$\rightarrow 41$	1.95E+11	$\rightarrow 38$	1.74E+11	$\rightarrow 47$	1.12E+11	$\rightarrow 49$	3.43E+12
162	2.95E+12	$\rightarrow 40$	2.61E+11	$\rightarrow 50$	1.49E+11	$\rightarrow 56$	6.22E+09	$\rightarrow 84$	5.24E+09	$\rightarrow 5$	3.38E+12
163	1.67E+12	$\rightarrow 47$	4.94E+11	$\rightarrow 35$	3.92E+11	$\rightarrow 55$	2.49E+11	$\rightarrow 46$	1.80E+11	$\rightarrow 38$	3.35E+12
164	1.69E+12	$\rightarrow 49$	7.50E+11	$\rightarrow 41$	3.63E+11	$\rightarrow 54$	2.07E+11	$\rightarrow 51$	2.05E+11	$\rightarrow 40$	3.32E+12
165	2.90E+12	$\rightarrow 2$	5.24E+11	$\rightarrow 27$	1.07E+11	$\rightarrow 24$	8.99E+10	$\rightarrow 56$	8.15E+10	$\rightarrow 47$	3.90E+12
166	3.37E+12	$\rightarrow 2$	5.78E+11	$\rightarrow 27$	1.50E+11	$\rightarrow 1$	7.78E+10	$\rightarrow 15$	7.47E+10	$\rightarrow 59$	4.40E+12
167	1.72E+12	$\rightarrow 33$	2.26E+09	$\rightarrow 96$	1.31E+09	$\rightarrow 109$	1.00E+09	$\rightarrow 91$	5.86E+08	$\rightarrow 24$	1.73E+12
168	6.47E+12	$\rightarrow 5$	9.41E+11	$\rightarrow 37$	6.01E+11	$\rightarrow 33$	1.07E+11	$\rightarrow 39$	5.74E+10	$\rightarrow 30$	8.21E+12
169	4.97E+12	$\rightarrow 5$	2.12E+12	$\rightarrow 4$	8.18E+11	$\rightarrow 37$	4.71E+11	$\rightarrow 34$	1.28E+11	$\rightarrow 33$	8.97E+12
170	4.23E+12	$\rightarrow 4$	2.62E+12	$\rightarrow 5$	5.76E+11	$\rightarrow 36$	5.43E+11	$\rightarrow 34$	3.77E+11	$\rightarrow 37$	8.68E+12
171	5.93E+12	$\rightarrow 4$	9.38E+11	$\rightarrow 36$	6.72E+11	$\rightarrow 34$	5.40E+10	$\rightarrow 28$	1.82E+10	$\rightarrow 32$	7.66E+12
172	2.88E+12	$\rightarrow 7$	1.20E+12	$\rightarrow 10$	9.05E+11	$\rightarrow 6$	6.66E+11	$\rightarrow 36$	5.59E+11	$\rightarrow 5$	7.23E+12
173	2.28E+12	$\rightarrow 9$	1.36E+12	$\rightarrow 10$	1.05E+12	$\rightarrow 8$	6.36E+11	$\rightarrow 44$	5.45E+11	$\rightarrow 7$	7.36E+12
174	9.12E+12	$\rightarrow 7$	1.38E+12	$\rightarrow 39$	1.69E+11	$\rightarrow 37$	2.65E+10	$\rightarrow 30$	2.58E+10	$\rightarrow 60$	1.08E+13
175	1.66E+12	$\rightarrow 51$	8.69E+11	$\rightarrow 50$	3.85E+11	$\rightarrow 49$	1.75E+11	$\rightarrow 54$	1.07E+11	$\rightarrow 40$	3.42E+12
176	2.51E+12	$\rightarrow 50$	6.57E+11	$\rightarrow 48$	1.99E+11	$\rightarrow 40$	4.13E+10	$\rightarrow 56$	9.08E+09	$\rightarrow 84$	3.42E+12
177	1.28E+12	$\rightarrow 52$	1.15E+12	$\rightarrow 51$	3.57E+11	$\rightarrow 55$	2.18E+11	$\rightarrow 49$	1.46E+11	$\rightarrow 50$	3.43E+12
178	2.01E+12	$\rightarrow 54$	3.83E+11	$\rightarrow 56$	3.20E+11	$\rightarrow 49$	3.09E+11	$\rightarrow 51$	2.33E+11	$\rightarrow 50$	3.38E+12
179	3.42E+12	$\rightarrow 48$	9.11E+08	$\rightarrow 33$	5.85E+07	$\rightarrow 167$	5.45E+05	$\rightarrow 96$	2.79E+05	$\rightarrow 109$	3.42E+12
180	5.39E+12	$\rightarrow 9$	1.10E+12	$\rightarrow 44$	7.28E+11	$\rightarrow 8$	4.82E+11	$\rightarrow 10$	2.75E+11	$\rightarrow 3$	8.71E+12
181	1.77E+12	$\rightarrow 52$	9.83E+11	$\rightarrow 53$	3.46E+11	$\rightarrow 51$	1.67E+11	$\rightarrow 59$	5.10E+10	$\rightarrow 47$	3.44E+12
182	2.92E+12	$\rightarrow 56$	2.26E+11	$\rightarrow 40$	3.84E+10	$\rightarrow 66$	1.00E+10	$\rightarrow 7$	8.05E+09	$\rightarrow 50$	3.21E+12
183	1.66E+12	$\rightarrow 55$	6.17E+11	$\rightarrow 54$	3.15E+11	$\rightarrow 52$	2.84E+11	$\rightarrow 51$	2.48E+11	$\rightarrow 47$	3.39E+12
184	2.64E+12	$\rightarrow 53$	7.46E+11	$\rightarrow 52$	9.98E+09	$\rightarrow 19$	8.79E+09	$\rightarrow 43$	7.77E+09	$\rightarrow 76$	3.45E+12
185	2.02E+12	$\rightarrow 59$	7.06E+11	$\rightarrow 55$	1.63E+11	$\rightarrow 47$	1.39E+11	$\rightarrow 52$	7.18E+10	$\rightarrow 53$	3.35E+12
186	3.87E+11	$\rightarrow 6$	3.07E+11	$\rightarrow 61$	2.59E+11	$\rightarrow 10$	2.28E+11	$\rightarrow 9$	1.18E+11	$\rightarrow 58$	1.68E+12
187	3.80E+11	$\rightarrow 10$	3.14E+11	$\rightarrow 60$	2.59E+11	$\rightarrow 7$	1.59E+11	$\rightarrow 58$	9.69E+10	$\rightarrow 6$	1.56E+12
188	7.60E+11	$\rightarrow 2$	3.31E+11	$\rightarrow 45$	3.30E+11	$\rightarrow 46$	2.27E+11	$\rightarrow 1$	1.02E+11	$\rightarrow 67$	1.89E+12
189	1.18E+12	$\rightarrow 2$	4.15E+11	$\rightarrow 46$	2.87E+11	$\rightarrow 1$	2.23E+11	$\rightarrow 45$	9.18E+10	$\rightarrow 69$	2.37E+12
190	1.20E+12	$\rightarrow 2$	6.04E+11	$\rightarrow 46$	1.03E+11	$\rightarrow 66$	6.68E+10	$\rightarrow 47$	1.94E+10	$\rightarrow 128$	2.09E+12
191	8.99E+11	$\rightarrow 2$	3.48E+11	$\rightarrow 1$	3.40E+11	$\rightarrow 45$	2.91E+11	$\rightarrow 46$	9.40E+10	$\rightarrow 71$	2.12E+12
192	5.31E+11	$\rightarrow 1$	4.50E+11	$\rightarrow 2$	4.13E+11	$\rightarrow 45$	1.76E+11	$\rightarrow 46$	1.02E+11	$\rightarrow 74$	1.85E+12
193	2.87E+12	$\rightarrow 8$	2.76E+12	$\rightarrow 9$	1.26E+12	$\rightarrow 6$	9.63E+11	$\rightarrow 10$	8.72E+11	$\rightarrow 57$	9.64E+12
194	4.69E+12	$\rightarrow 6$	1.24E+12	$\rightarrow 58$	3.99E+11	$\rightarrow 7$	2.08E+11	$\rightarrow 60$	1.85E+11	$\rightarrow 61$	6.88E+12
195	3.25E+12	$\rightarrow 7$	1.62E+12	$\rightarrow 60$	2.32E+10	$\rightarrow 39$	2.21E+10	$\rightarrow 80$	2.18E+10	$\rightarrow 5$	4.98E+12
196	7.52E+12	$\rightarrow 10$	1.22E+12	$\rightarrow 61$	3.73E+11	$\rightarrow 7$	2.70E+11	$\rightarrow 60$	1.62E+11	$\rightarrow 6$	9.78E+12
197	4.61E+12	$\rightarrow 8$	1.14E+12	$\rightarrow 10$	7.05E+11	$\rightarrow 57$	3.55E+11	$\rightarrow 62$	3.05E+11	$\rightarrow 6$	7.76E+12
198	3.19E+12	$\rightarrow 10$	2.51E+12	$\rightarrow 9$	5.71E+11	$\rightarrow 63$	4.01E+11	$\rightarrow 61$	3.69E+11	$\rightarrow 62$	7.73E+12
199	2.70E+12	$\rightarrow 69$	4.36E+11	$\rightarrow 67$	1.22E+11	$\rightarrow 71$	4.26E+10	$\rightarrow 47$	4.03E+10	$\rightarrow 55$	3.45E+12
200	2.85E+12	$\rightarrow 71$	3.80E+11	$\rightarrow 66$	4.97E+10	$\rightarrow 54$	4.48E+10	$\rightarrow 67$	2.71E+10	$\rightarrow 49$	3.44E+12
201	2.91E+12	$\rightarrow 67$	1.00E+11	$\rightarrow 71$	1.00E+11	$\rightarrow 66$	5.76E+10	$\rightarrow 54$	5.03E+10	$\rightarrow 95$	3.35E+12
202	3.17E+12	$\rightarrow 66$	7.29E+10	$\rightarrow 100$	5.78E+10	$\rightarrow 56$	4.15E+10	$\rightarrow 84$	1.32E+10	$\rightarrow 132$	3.36E+12
203	2.07E+12	$\rightarrow 73$	4.77E+11	$\rightarrow 69$	4.03E+11	$\rightarrow 74$	2.56E+11	$\rightarrow 70$	6.27E+10	$\rightarrow 75$	3.46E+12
204	2.29E+12	$\rightarrow 74$	4.88E+11	$\rightarrow 71$	4.65E+11	$\rightarrow 75$	4.61E+10	$\rightarrow 69$	2.50E+10	$\rightarrow 77$	3.45E+12
205	5.26E+11	$\rightarrow 11$	2.73E+11	$\rightarrow 75$	1.81E+11	$\rightarrow 70$	1.60E+11	$\rightarrow 12$	6.46E+10	$\rightarrow 77$	1.44E+12
206	1.75E+12	$\rightarrow 3$	3.72E+11	$\rightarrow 62$	3.39E+11	$\rightarrow 8$	2.37E+11	$\rightarrow 63$	1.50E+11	$\rightarrow 9$	3.19E+12
207	5.28E+11	$\rightarrow 11$	2.76E+11	$\rightarrow 78$	8.63E+10	$\rightarrow 77$	7.54E+10	$\rightarrow 13$	6.10E+10	$\rightarrow 82$	1.37E+12
208	9.97E+11	$\rightarrow 12$	3.65E+11	$\rightarrow 14$	1.81E+11	$\rightarrow 82$	8.39E+10	$\rightarrow 101$	7.40E+10	$\rightarrow 79$	2.12E+12
209	1.98E+12	$\rightarrow 3$	3.67E+11	$\rightarrow 62$	3.00E+11	$\rightarrow 8$	2.48E+11	$\rightarrow 63$	1.22E+11	$\rightarrow 9$	3.28E+12
210	8.41E+11	$\rightarrow 11$	2.88E+11	$\rightarrow 84$	1.44E+11	$\rightarrow 13$	1.27E+11	$\rightarrow 81$	1.01E+11	$\rightarrow 86$	1.75E+12
211	1.36E+12	$\rightarrow 4$	4.46E+11	$\rightarrow 10$	4.25E+11	$\rightarrow 64$	3.54E+11	$\rightarrow 8$	1.56E+11	$\rightarrow 9$	3.45E+12
212	7.59E+11	$\rightarrow 13$	4.05E+11	$\rightarrow 14$	2.28E+11	$\rightarrow 12$	2.07E+11	$\rightarrow 15$	1.72E+11	$\rightarrow 88$	2.37E+12
213	1.18E+12	$\rightarrow 70$	4.15E+11	$\rightarrow 11$	2.32E+11	$\rightarrow 12$	1.79E+11	$\rightarrow 75$	1.55E+11	$\rightarrow 73$	2.53E+12
214	1.59E+12	$\rightarrow 4$	5.08E+11	$\rightarrow 8$	4.88E+11	$\rightarrow 64$	1.98E+11	$\rightarrow 9$	1.61E+11	$\rightarrow 68$	3.36E+12
215	2.05E+12	$\rightarrow 11$	1.14E+12	$\rightarrow 75$	8.97E+11	$\rightarrow 12$	2.75E+11	$\rightarrow 74$	1.71E+11	$\rightarrow 77$	4.66E+12
216	2.16E+12	$\rightarrow 4$	6.68E+11	$\rightarrow 64$	1.52E+11	$\rightarrow 10$	9.15E+10	$\rightarrow 91$	1.07E+10	$\rightarrow 61$	3.17E+12
217	8.94E+11	$\rightarrow 4$	8.84E+11	$\rightarrow 8$	3.81E+11	$\rightarrow 9$	3.34E+11	$\rightarrow 3$	3.23E+11	$\rightarrow 68$	3.47E+12
218	1.11E+12	$\rightarrow 8$	4.87E+11	$\rightarrow 4$	4.43E+11	$\rightarrow 9$	3.83E+11	$\rightarrow 68$	3.53E+11	$\rightarrow 3$	3.58E+12
219	2.83E+12	$\rightarrow 85$	1.61E+11	$\rightarrow 87$	1.32E+11	$\rightarrow 92$	8.57E+10	$\rightarrow 111$	3.26E+10	$\rightarrow 110$	3.39E+12
220	2.52E+12	$\rightarrow 87$	3.72E+11	$\rightarrow 93$	2.12E+11	$\rightarrow 110$	1.22E+11	$\rightarrow 103$	3.03E+10	$\rightarrow 99$	3.32E+12
221	1.57E+12	$\rightarrow 5$	5.10E+11	$\rightarrow 65$	4.16E+11	$\rightarrow 10$	2.08E+11	$\rightarrow 6$	1.75E+11	$\rightarrow 7$	3.32E+12
222	2.07E+12	$\rightarrow 5$	7.01E+11	$\rightarrow 65$	1.31E+11	$\rightarrow 7$	8.64E+10	$\rightarrow 97$	2.17E+10	$\rightarrow 96$	3.05E+12
223	2.31E+12	$\rightarrow 5$	6.29E+11	$\rightarrow 65$	1.26E+11	$\rightarrow 7$	1.01E+11	$\rightarrow 4$	5.04E+10	$\rightarrow 106$	3.45E+12
224	1.31E+12	$\rightarrow 11$	8.28E+11	$\rightarrow 76$	3.60E+11	$\rightarrow 77$	2.65E+11	$\rightarrow 14$	2.39E+11	$\rightarrow 15$	3.80E+12
225	1.48E+12	$\rightarrow 78$	4.62E+11	$\rightarrow 13$	1.98E+11	$\rightarrow 81$	8.97E+09	$\rightarrow 102$	4.58E+09	$\rightarrow 146$	2.18E+12
226	8.74E+11	$\rightarrow 76$	5.55E+11	$\rightarrow 11$	4.87E+11	$\rightarrow 79$	2.74E+11	$\rightarrow 14$	1.25E+11	$\rightarrow 77$	2.71E+12
227	1.20E+12	$\rightarrow 6$	1.09E+12	$\rightarrow 10$	5.32E+11	$\rightarrow 72$	1.64E+11	$\rightarrow 8$	1.63E+11	$\rightarrow 4$	3.60E+12
228	2.99E+12	$\rightarrow 11$	9.03E+11	$\rightarrow 77$	4.49E+11	$\rightarrow 78$	1.41E+11	$\rightarrow 75$	1.28E+11	$\rightarrow 13$	5.01E+12
229	1.14E+12	$\rightarrow 10$	8.27E+11	$\rightarrow 6$	6.58E+11	$\rightarrow 5$	4.51E+11	$\rightarrow 72$	1.67E+11	$\rightarrow 65$	3.58E+12
230	1.56E+12	$\rightarrow 10$	4.70E+11	$\rightarrow 6$	3.97E+11	$\rightarrow 72$	2.24E+11	$\rightarrow 8$	1.34E+11	$\rightarrow 4$	3.32E+12
231	1.93E+12	$\rightarrow 12$	1.18E+12	$\rightarrow 14$	9.48E+11	$\rightarrow 79$	7.57E+11	$\rightarrow 11$	1.65E+11	$\rightarrow 82$	5.64E+12
232	4.59E+12	$\rightarrow 12$	1.27E+12	$\rightarrow 11$	1.18E+12	$\rightarrow 82$	1.03E+11	$\rightarrow 86$	1.02E+11	$\rightarrow 77$	7.66E+12
233	2.35E+12	$\rightarrow 92$	2.10E+11	$\rightarrow 93$	1.53E+11	$\rightarrow 85$	1.48E+11	$\rightarrow 106$	1.42E+11	$\rightarrow 87$	3.42E+12
234	1.43E+12	$\rightarrow 99$	7.05E+11	$\rightarrow 93$	4.36E+11	$\rightarrow 91$	3.32E+11	$\rightarrow 87$	3.01E+11	$\rightarrow 103$	3.37E+12
235	3.00E+12	$\rightarrow 91$	1.47E+11	$\rightarrow 96$	1.00E+11	$\rightarrow 117$	6.89E+10	$\rightarrow 109$	1.37E+10	$\rightarrow 113$	3.35E+12
236	1.04E+12	$\rightarrow 99$	8.11E+11	$\rightarrow 93$	8.03E+11	$\rightarrow 110$	3.94E+11	$\rightarrow 87$	1.41E+11	$\rightarrow 116$	3.27E+12
237	2.23E+12	$\rightarrow 94$	5.70E+11	$\rightarrow 92$	1.46E+11	$\rightarrow 98$	1.38E+11	$\rightarrow 106$	1.20E+11	$\rightarrow 108$	3.42E+12
238	1.03E+12	$\rightarrow 81$	5.08E+11	$\rightarrow 84$	1.30E+11	$\rightarrow 78$	1.12E+10	$\rightarrow 67$	7.85E+09	$\rightarrow 66$	1.72E+12
239	1.68E+12	$\rightarrow 84$	2.08E+10	$\rightarrow 66$	6.64E+09	$\rightarrow 167$	5.29E+09	$\rightarrow 50$	4.17E+09	$\rightarrow 148$	1.72E+12
240	2.03E+12	$\rightarrow 98$	5.88E+11	$\rightarrow 111$	2.91E+11	$\rightarrow 99$	1.46E+11	$\rightarrow 106$	6.08E+10	$\rightarrow 103$	3.35E+12
241	1.95E+12	$\rightarrow 13$	5.57E+11	$\rightarrow 11$	3.00E+11	$\rightarrow 15$	2.55E+11	$\rightarrow 102$	2.12E+11	$\rightarrow 100$	3.95E+12
242	1.01E+12	$\rightarrow 15$	2.40E+11	$\rightarrow 95$	2.38E+11	$\rightarrow 112$	1.50E+11	$\rightarrow 11$	1.47E+11	$\rightarrow 12$	2.15E+12
243	3.18E+12	$\rightarrow 11$	9.23E+11	$\rightarrow 12$	6.45E+11	$\rightarrow 81$	3.36E+11	$\rightarrow 15$	3.17E+11	$\rightarrow 89$	6.18E+12
244	7.13E+12	$\rightarrow 11$	5.68E+11	$\rightarrow 86$	4.60E+11	$\rightarrow 13$	3.71E+11	$\rightarrow 89$	3.40E+11	$\rightarrow 81$	9.41E+12
245	8.40E+12	$\rightarrow 11$	8.92E+11	$\rightarrow 86$	3.29E+11	$\rightarrow 14$	3.17E+11	$\rightarrow 89$	2.08E+11	$\rightarrow 77$	1.04E+13
246	4.31E+12	$\rightarrow 14$	7.14E+11	$\rightarrow 11$	6.35E+11	$\rightarrow 90$	5.52E+11	$\rightarrow 15$	3.16E+11	$\rightarrow 79$	7.48E+12
247	7.90E+12	$\rightarrow 13$	1.26E+12	$\rightarrow 88$	1.91E+11	$\rightarrow 102$	8.65E+10	$\rightarrow 84$	3.87E+10	$\rightarrow 81$	9.56E+12
248	4.79E+12	$\rightarrow 14$	8.59E+11	$\rightarrow 15$	4.97E+11	$\rightarrow 90$	4.83E+11	$\rightarrow 13$	2.75E+11	$\rightarrow 82$	8.05E+12
249	3.70E+12	$\rightarrow 12$	1.82E+12	$\rightarrow 13$	7.88E+11	$\rightarrow 15$	4.88E+11	$\rightarrow 89$	4.54E+11	$\rightarrow 86$	7.90E+12
250	2.30E+12	$\rightarrow 96$	3.38E+11	$\rightarrow 97$	2.59E+11	$\rightarrow 109$	2.45E+11	$\rightarrow 91$	1.24E+11	$\rightarrow 117$	3.34E+12
251	3.34E+12	$\rightarrow 97$	1.24E+10	$\rightarrow 114$	5.59E+09	$\rightarrow 179$	3.76E+09	$\rightarrow 162$	8.49E+08	$\rightarrow 84$	3.36E+12
252	2.14E+12	$\rightarrow 108$	6.74E+11	$\rightarrow 106$	2.33E+11	$\rightarrow 104$	1.27E+11	$\rightarrow 107$	8.01E+10	$\rightarrow 94$	3.41E+12
253	1.15E+12	$\rightarrow 103$	9.61E+11	$\rightarrow 96$	7.24E+11	$\rightarrow 93$	3.10E+11	$\rightarrow 110$	6.40E+10	$\rightarrow 91$	3.39E+12
254	1.64E+12	$\rightarrow 106$	6.34E+11	$\rightarrow 108$	3.28E+11	$\rightarrow 103$	1.91E+11	$\rightarrow 104$	1.82E+11	$\rightarrow 92$	3.42E+12
255	1.22E+12	$\rightarrow 106$	1.06E+12	$\rightarrow 103$	4.29E+11	$\rightarrow 93$	2.33E+11	$\rightarrow 98$	1.62E+11	$\rightarrow 96$	3.41E+12
256	1.92E+12	$\rightarrow 109$	5.12E+11	$\rightarrow 117$	3.68E+11	$\rightarrow 96$	2.96E+11	$\rightarrow 97$	8.04E+10	$\rightarrow 91$	3.25E+12
257	1.06E+12	$\rightarrow 107$	5.23E+11	$\rightarrow 111$	5.04E+11	$\rightarrow 104$	3.88E+11	$\rightarrow 108$	3.84E+11	$\rightarrow 98$	3.38E+12
258	1.36E+12	$\rightarrow 110$	6.31E+11	$\rightarrow 103$	4.29E+11	$\rightarrow 109$	2.64E+11	$\rightarrow 99$	2.30E+11	$\rightarrow 93$	3.29E+12
259	1.69E+12	$\rightarrow 111$	4.24E+11	$\rightarrow 98$	3.37E+11	$\rightarrow 110$	1.85E+11	$\rightarrow 103$	1.38E+11	$\rightarrow 93$	3.32E+12
260	3.03E+11	$\rightarrow 2$	2.07E+11	$\rightarrow 18$	1.50E+11	$\rightarrow 1$	1.44E+11	$\rightarrow 128$	9.96E+10	$\rightarrow 17$	9.93E+11
261	1.16E+12	$\rightarrow 6$	9.44E+11	$\rightarrow 10$	6.04E+11	$\rightarrow 83$	1.96E+11	$\rightarrow 7$	8.00E+10	$\rightarrow 113$	3.25E+12
262	1.78E+12	$\rightarrow 7$	4.66E+11	$\rightarrow 80$	4.31E+11	$\rightarrow 6$	3.63E+11	$\rightarrow 10$	1.93E+11	$\rightarrow 83$	3.61E+12
263	2.10E+12	$\rightarrow 7$	6.90E+11	$\rightarrow 80$	1.38E+11	$\rightarrow 5$	8.80E+10	$\rightarrow 114$	1.54E+10	$\rightarrow 117$	3.09E+12
264	2.21E+12	$\rightarrow 7$	6.18E+11	$\rightarrow 80$	3.37E+11	$\rightarrow 10$	1.06E+11	$\rightarrow 5$	7.47E+10	$\rightarrow 83$	3.53E+12
265	1.80E+12	$\rightarrow 6$	8.07E+11	$\rightarrow 10$	5.48E+11	$\rightarrow 83$	6.46E+10	$\rightarrow 72$	5.39E+10	$\rightarrow 122$	3.47E+12
266	3.92E+11	$\rightarrow 16$	1.56E+11	$\rightarrow 126$	6.32E+10	$\rightarrow 129$	6.03E+10	$\rightarrow 20$	5.22E+10	$\rightarrow 8$	7.71E+11
267	3.79E+11	$\rightarrow 16$	1.49E+11	$\rightarrow 126$	5.43E+10	$\rightarrow 130$	5.20E+10	$\rightarrow 21$	4.90E+10	$\rightarrow 9$	7.54E+11
268	1.03E+12	$\rightarrow 10$	7.81E+11	$\rightarrow 6$	6.20E+11	$\rightarrow 7$	4.34E+11	$\rightarrow 83$	1.56E+11	$\rightarrow 80$	3.27E+12
269	1.39E+12	$\rightarrow 95$	8.68E+11	$\rightarrow 13$	2.34E+11	$\rightarrow 100$	5.80E+10	$\rightarrow 102$	1.09E+10	$\rightarrow 67$	2.59E+12
270	2.39E+12	$\rightarrow 1$	6.84E+11	$\rightarrow 17$	4.61E+11	$\rightarrow 2$	2.71E+11	$\rightarrow 127$	1.36E+11	$\rightarrow 18$	4.09E+12
271	1.66E+12	$\rightarrow 100$	2.94E+10	$\rightarrow 66$	5.24E+09	$\rightarrow 84$	3.40E+09	$\rightarrow 167$	2.89E+09	$\rightarrow 195$	1.70E+12
272	2.82E+12	$\rightarrow 2$	8.16E+11	$\rightarrow 18$	3.30E+11	$\rightarrow 128$	2.13E+10	$\rightarrow 12$	2.08E+10	$\rightarrow 27$	4.06E+12
273	4.61E+12	$\rightarrow 13$	2.39E+12	$\rightarrow 12$	7.21E+11	$\rightarrow 102$	4.65E+11	$\rightarrow 101$	1.89E+11	$\rightarrow 88$	8.97E+12
274	4.59E+12	$\rightarrow 12$	1.41E+12	$\rightarrow 13$	8.77E+11	$\rightarrow 101$	3.06E+11	$\rightarrow 14$	2.45E+11	$\rightarrow 102$	8.20E+12
275	6.58E+12	$\rightarrow 13$	9.55E+11	$\rightarrow 102$	3.43E+11	$\rightarrow 100$	2.07E+11	$\rightarrow 95$	1.19E+11	$\rightarrow 88$	8.25E+12
276	2.64E+12	$\rightarrow 12$	1.74E+12	$\rightarrow 14$	8.74E+11	$\rightarrow 105$	4.67E+11	$\rightarrow 101$	2.08E+11	$\rightarrow 90$	6.19E+12
277	1.09E+12	$\rightarrow 20$	5.72E+11	$\rightarrow 129$	7.71E+10	$\rightarrow 21$	4.09E+10	$\rightarrow 130$	6.82E+09	$\rightarrow 6$	1.80E+12
278	1.16E+12	$\rightarrow 21$	6.12E+11	$\rightarrow 130$	6.46E+09	$\rightarrow 7$	4.88E+09	$\rightarrow 2$	1.67E+09	$\rightarrow 116$	1.79E+12
279	9.86E+11	$\rightarrow 131$	3.64E+10	$\rightarrow 132$	2.97E+09	$\rightarrow 67$	1.17E+09	$\rightarrow 20$	3.04E+08	$\rightarrow 54$	1.03E+12
280	1.02E+12	$\rightarrow 132$	3.55E+09	$\rightarrow 66$	1.29E+09	$\rightarrow 21$	3.66E+08	$\rightarrow 56$	1.53E+08	$\rightarrow 100$	1.03E+12
281	4.37E+12	$\rightarrow 15$	1.45E+12	$\rightarrow 12$	5.80E+11	$\rightarrow 112$	5.18E+11	$\rightarrow 101$	4.36E+11	$\rightarrow 11$	8.32E+12
282	7.78E+12	$\rightarrow 15$	2.09E+12	$\rightarrow 12$	8.97E+11	$\rightarrow 112$	4.91E+11	$\rightarrow 95$	1.72E+11	$\rightarrow 101$	1.18E+13
283	1.69E+12	$\rightarrow 113$	5.73E+11	$\rightarrow 117$	5.55E+11	$\rightarrow 114$	5.24E+11	$\rightarrow 109$	3.66E+10	$\rightarrow 96$	3.41E+12
284	1.60E+12	$\rightarrow 116$	6.97E+11	$\rightarrow 117$	4.25E+11	$\rightarrow 120$	2.42E+11	$\rightarrow 109$	2.08E+11	$\rightarrow 99$	3.34E+12
285	1.92E+12	$\rightarrow 115$	9.20E+11	$\rightarrow 116$	1.70E+11	$\rightarrow 120$	1.11E+11	$\rightarrow 99$	8.93E+10	$\rightarrow 117$	3.39E+12
286	6.77E+12	$\rightarrow 15$	8.49E+11	$\rightarrow 112$	6.28E+11	$\rightarrow 13$	3.42E+11	$\rightarrow 14$	2.70E+11	$\rightarrow 105$	9.78E+12
287	1.99E+12	$\rightarrow 120$	6.21E+11	$\rightarrow 113$	3.48E+11	$\rightarrow 116$	1.14E+11	$\rightarrow 110$	7.37E+10	$\rightarrow 109$	3.34E+12
288	1.50E+12	$\rightarrow 117$	1.41E+12	$\rightarrow 113$	2.52E+11	$\rightarrow 109$	8.75E+10	$\rightarrow 114$	9.43E+09	$\rightarrow 91$	3.27E+12
289	3.27E+12	$\rightarrow 114$	1.82E+10	$\rightarrow 97$	3.43E+09	$\rightarrow 202$	3.00E+09	$\rightarrow 179$	8.35E+08	$\rightarrow 100$	3.29E+12
290	1.45E+12	$\rightarrow 115$	1.29E+12	$\rightarrow 118$	2.53E+11	$\rightarrow 116$	1.39E+11	$\rightarrow 107$	7.92E+10	$\rightarrow 122$	3.44E+12
291	1.93E+12	$\rightarrow 122$	5.78E+11	$\rightarrow 120$	5.22E+11	$\rightarrow 116$	6.78E+10	$\rightarrow 113$	6.76E+10	$\rightarrow 110$	3.37E+12
292	1.76E+12	$\rightarrow 121$	7.04E+11	$\rightarrow 118$	4.08E+11	$\rightarrow 115$	3.33E+11	$\rightarrow 122$	6.47E+10	$\rightarrow 104$	3.41E+12
293	1.29E+12	$\rightarrow 121$	1.24E+12	$\rightarrow 122$	3.75E+11	$\rightarrow 118$	1.63E+11	$\rightarrow 107$	1.25E+11	$\rightarrow 116$	3.40E+12
294	4.38E+11	$\rightarrow 123$	2.16E+11	$\rightarrow 119$	1.20E+11	$\rightarrow 14$	7.60E+10	$\rightarrow 15$	3.51E+10	$\rightarrow 112$	9.63E+11
295	2.04E+12	$\rightarrow 9$	4.61E+11	$\rightarrow 8$	4.58E+11	$\rightarrow 104$	2.23E+11	$\rightarrow 107$	1.36E+11	$\rightarrow 125$	3.41E+12
296	1.66E+12	$\rightarrow 9$	6.41E+11	$\rightarrow 8$	4.30E+11	$\rightarrow 104$	2.27E+11	$\rightarrow 107$	1.15E+11	$\rightarrow 124$	3.20E+12
297	3.73E+12	$\rightarrow 15$	1.64E+12	$\rightarrow 123$	9.80E+10	$\rightarrow 12$	3.35E+10	$\rightarrow 2$	1.76E+10	$\rightarrow 13$	5.60E+12
298	4.92E+12	$\rightarrow 14$	1.35E+12	$\rightarrow 119$	7.44E+11	$\rightarrow 15$	2.76E+11	$\rightarrow 123$	2.02E+10	$\rightarrow 90$	7.39E+12
299	2.92E+12	$\rightarrow 125$	2.15E+11	$\rightarrow 124$	8.06E+10	$\rightarrow 111$	3.87E+10	$\rightarrow 115$	2.54E+10	$\rightarrow 122$	3.35E+12
300	3.18E+12	$\rightarrow 124$	7.59E+10	$\rightarrow 120$	3.01E+10	$\rightarrow 110$	2.08E+10	$\rightarrow 116$	1.38E+10	$\rightarrow 202$	3.36E+12
301	2.49E+11	$\rightarrow 4$	1.70E+11	$\rightarrow 28$	1.22E+11	$\rightarrow 137$	8.74E+10	$\rightarrow 6$	8.72E+10	$\rightarrow 25$	9.85E+11
302	1.83E+11	$\rightarrow 5$	1.71E+11	$\rightarrow 3$	1.41E+11	$\rightarrow 30$	1.12E+11	$\rightarrow 141$	6.11E+10	$\rightarrow 31$	1.02E+12
303	4.89E+11	$\rightarrow 1$	3.36E+11	$\rightarrow 19$	1.52E+11	$\rightarrow 133$	6.03E+10	$\rightarrow 144$	5.01E+10	$\rightarrow 23$	1.21E+12
304	3.68E+11	$\rightarrow 6$	1.61E+11	$\rightarrow 8$	1.38E+11	$\rightarrow 32$	1.10E+11	$\rightarrow 143$	9.62E+10	$\rightarrow 29$	1.14E+12
305	4.04E+11	$\rightarrow 1$	3.40E+11	$\rightarrow 19$	1.47E+11	$\rightarrow 133$	5.05E+10	$\rightarrow 146$	3.97E+10	$\rightarrow 23$	1.09E+12
306	5.33E+11	$\rightarrow 1$	2.75E+11	$\rightarrow 22$	1.78E+11	$\rightarrow 2$	1.16E+11	$\rightarrow 134$	9.53E+10	$\rightarrow 23$	1.44E+12
307	6.52E+11	$\rightarrow 25$	5.23E+11	$\rightarrow 3$	2.68E+11	$\rightarrow 136$	2.63E+11	$\rightarrow 4$	1.77E+11	$\rightarrow 8$	2.30E+12
308	3.70E+11	$\rightarrow 22$	1.50E+11	$\rightarrow 134$	1.44E+11	$\rightarrow 2$	3.09E+10	$\rightarrow 150$	2.85E+10	$\rightarrow 43$	8.29E+11
309	3.76E+11	$\rightarrow 22$	1.52E+11	$\rightarrow 134$	1.46E+11	$\rightarrow 2$	4.81E+10	$\rightarrow 148$	3.83E+10	$\rightarrow 40$	8.18E+11
310	2.00E+12	$\rightarrow 4$	6.21E+11	$\rightarrow 28$	5.85E+11	$\rightarrow 6$	2.84E+11	$\rightarrow 137$	1.52E+11	$\rightarrow 26$	3.79E+12
311	1.80E+12	$\rightarrow 1$	3.16E+11	$\rightarrow 23$	1.43E+11	$\rightarrow 135$	6.20E+10	$\rightarrow 153$	5.02E+10	$\rightarrow 19$	2.54E+12
312	1.35E+12	$\rightarrow 1$	2.45E+11	$\rightarrow 23$	1.11E+11	$\rightarrow 135$	8.98E+10	$\rightarrow 22$	5.39E+10	$\rightarrow 14$	2.12E+12
313	8.51E+11	$\rightarrow 35$	5.13E+11	$\rightarrow 144$	1.18E+11	$\rightarrow 47$	7.13E+10	$\rightarrow 42$	3.58E+10	$\rightarrow 153$	1.79E+12
314	5.31E+11	$\rightarrow 41$	5.03E+11	$\rightarrow 146$	4.74E+11	$\rightarrow 38$	6.68E+10	$\rightarrow 147$	5.92E+10	$\rightarrow 54$	1.75E+12
315	9.65E+11	$\rightarrow 151$	3.56E+10	$\rightarrow 152$	4.73E+09	$\rightarrow 163$	1.19E+09	$\rightarrow 165$	8.72E+08	$\rightarrow 35$	1.01E+12
316	1.00E+12	$\rightarrow 152$	3.68E+09	$\rightarrow 160$	1.66E+09	$\rightarrow 164$	1.14E+09	$\rightarrow 91$	7.80E+08	$\rightarrow 155$	1.01E+12
317	5.23E+11	$\rightarrow 5$	4.96E+11	$\rightarrow 26$	2.72E+11	$\rightarrow 4$	2.06E+11	$\rightarrow 138$	1.78E+11	$\rightarrow 30$	2.28E+12
318	2.22E+12	$\rightarrow 3$	4.68E+11	$\rightarrow 4$	3.26E+11	$\rightarrow 31$	2.34E+11	$\rightarrow 26$	1.61E+11	$\rightarrow 32$	4.22E+12
319	1.81E+12	$\rightarrow 5$	7.44E+11	$\rightarrow 30$	3.47E+11	$\rightarrow 7$	3.33E+11	$\rightarrow 141$	9.66E+10	$\rightarrow 37$	3.36E+12
320	3.88E+12	$\rightarrow 3$	6.09E+11	$\rightarrow 31$	2.08E+11	$\rightarrow 140$	1.34E+11	$\rightarrow 9$	1.10E+11	$\rightarrow 4$	5.37E+12
321	1.85E+12	$\rightarrow 8$	6.08E+11	$\rightarrow 29$	4.33E+11	$\rightarrow 6$	2.29E+11	$\rightarrow 142$	6.20E+10	$\rightarrow 26$	3.51E+12
322	2.60E+12	$\rightarrow 6$	6.78E+11	$\rightarrow 4$	6.29E+11	$\rightarrow 32$	2.81E+11	$\rightarrow 143$	1.34E+11	$\rightarrow 5$	4.58E+12
323	7.41E+11	$\rightarrow 43$	4.24E+11	$\rightarrow 150$	2.54E+11	$\rightarrow 42$	1.56E+11	$\rightarrow 149$	5.86E+10	$\rightarrow 35$	1.78E+12
324	6.14E+11	$\rightarrow 38$	4.05E+11	$\rightarrow 147$	3.05E+11	$\rightarrow 41$	1.24E+11	$\rightarrow 49$	9.00E+10	$\rightarrow 40$	1.79E+12
325	1.01E+12	$\rightarrow 40$	5.91E+11	$\rightarrow 148$	7.23E+10	$\rightarrow 50$	5.33E+10	$\rightarrow 56$	8.25E+09	$\rightarrow 174$	1.75E+12
326	8.10E+11	$\rightarrow 42$	4.42E+11	$\rightarrow 149$	1.31E+11	$\rightarrow 41$	9.48E+10	$\rightarrow 147$	8.13E+10	$\rightarrow 38$	1.79E+12
327	1.33E+11	$\rightarrow 5$	1.26E+11	$\rightarrow 33$	1.04E+11	$\rightarrow 6$	8.73E+10	$\rightarrow 155$	6.91E+10	$\rightarrow 37$	8.65E+11
328	5.93E+11	$\rightarrow 47$	4.97E+11	$\rightarrow 153$	1.84E+11	$\rightarrow 35$	1.46E+11	$\rightarrow 55$	8.97E+10	$\rightarrow 46$	1.77E+12
329	9.16E+11	$\rightarrow 160$	5.69E+10	$\rightarrow 164$	2.76E+10	$\rightarrow 162$	4.76E+09	$\rightarrow 152$	6.34E+08	$\rightarrow 38$	1.01E+12
330	6.02E+11	$\rightarrow 49$	4.98E+11	$\rightarrow 156$	2.26E+11	$\rightarrow 41$	1.21E+11	$\rightarrow 54$	8.07E+10	$\rightarrow 51$	1.72E+12
331	8.30E+11	$\rightarrow 159$	1.13E+11	$\rightarrow 161$	3.64E+10	$\rightarrow 158$	2.63E+10	$\rightarrow 163$	3.24E+09	$\rightarrow 160$	1.02E+12
332	1.00E+12	$\rightarrow 162$	1.27E+09	$\rightarrow 97$	1.14E+09	$\rightarrow 40$	8.24E+08	$\rightarrow 182$	5.63E+08	$\rightarrow 176$	1.01E+12
333	8.49E+11	$\rightarrow 161$	8.00E+10	$\rightarrow 164$	6.19E+10	$\rightarrow 163$	1.67E+10	$\rightarrow 160$	2.20E+09	$\rightarrow 165$	1.02E+12
334	8.36E+11	$\rightarrow 163$	7.54E+10	$\rightarrow 160$	4.09E+10	$\rightarrow 161$	3.78E+10	$\rightarrow 165$	3.90E+09	$\rightarrow 151$	1.01E+12
335	9.03E+11	$\rightarrow 164$	5.66E+10	$\rightarrow 162$	3.98E+10	$\rightarrow 160$	1.34E+09	$\rightarrow 152$	1.12E+09	$\rightarrow 155$	1.01E+12
336	4.00E+11	$\rightarrow 7$	1.35E+11	$\rightarrow 39$	1.09E+11	$\rightarrow 9$	8.94E+10	$\rightarrow 165$	8.83E+10	$\rightarrow 10$	1.21E+12
337	4.97E+11	$\rightarrow 2$	2.78E+11	$\rightarrow 24$	1.10E+11	$\rightarrow 27$	1.07E+11	$\rightarrow 139$	4.63E+10	$\rightarrow 145$	1.21E+12
338	3.58E+11	$\rightarrow 2$	3.21E+11	$\rightarrow 24$	1.24E+11	$\rightarrow 139$	7.53E+10	$\rightarrow 27$	3.16E+10	$\rightarrow 145$	1.06E+12
339	3.88E+11	$\rightarrow 24$	1.52E+11	$\rightarrow 139$	4.47E+10	$\rightarrow 167$	3.65E+10	$\rightarrow 48$	1.27E+10	$\rightarrow 168$	6.66E+11
340	1.21E+12	$\rightarrow 2$	2.59E+11	$\rightarrow 27$	1.07E+11	$\rightarrow 145$	1.07E+11	$\rightarrow 24$	4.06E+10	$\rightarrow 139$	1.93E+12
341	1.40E+12	$\rightarrow 2$	3.00E+11	$\rightarrow 27$	1.24E+11	$\rightarrow 145$	7.28E+10	$\rightarrow 24$	5.15E+10	$\rightarrow 15$	2.14E+12
342	1.65E+12	$\rightarrow 2$	3.37E+11	$\rightarrow 27$	1.42E+11	$\rightarrow 145$	4.50E+10	$\rightarrow 15$	3.86E+10	$\rightarrow 59$	2.36E+12
343	8.48E+11	$\rightarrow 33$	3.38E+11	$\rightarrow 155$	1.46E+10	$\rightarrow 179$	1.88E+09	$\rightarrow 176$	1.45E+09	$\rightarrow 96$	1.21E+12
344	2.63E+12	$\rightarrow 5$	4.58E+11	$\rightarrow 37$	3.04E+11	$\rightarrow 33$	2.00E+11	$\rightarrow 157$	1.17E+11	$\rightarrow 155$	3.84E+12
345	2.09E+12	$\rightarrow 5$	9.77E+11	$\rightarrow 4$	4.06E+11	$\rightarrow 37$	2.41E+11	$\rightarrow 34$	1.77E+11	$\rightarrow 157$	4.37E+12
346	1.94E+12	$\rightarrow 4$	1.16E+12	$\rightarrow 5$	2.92E+11	$\rightarrow 34$	2.75E+11	$\rightarrow 36$	1.91E+11	$\rightarrow 37$	4.36E+12
347	2.69E+12	$\rightarrow 4$	4.74E+11	$\rightarrow 36$	3.46E+11	$\rightarrow 34$	2.05E+11	$\rightarrow 154$	1.20E+11	$\rightarrow 158$	3.91E+12
348	1.28E+12	$\rightarrow 7$	7.06E+11	$\rightarrow 10$	3.27E+11	$\rightarrow 36$	3.17E+11	$\rightarrow 5$	2.84E+11	$\rightarrow 6$	3.79E+12
349	1.14E+12	$\rightarrow 9$	6.56E+11	$\rightarrow 10$	2.97E+11	$\rightarrow 44$	2.78E+11	$\rightarrow 8$	2.50E+11	$\rightarrow 7$	3.80E+12
350	4.27E+12	$\rightarrow 7$	7.11E+11	$\rightarrow 39$	2.77E+11	$\rightarrow 165$	6.78E+10	$\rightarrow 37$	3.26E+10	$\rightarrow 157$	5.48E+12
351	5.94E+11	$\rightarrow 51$	4.00E+11	$\rightarrow 169$	3.23E+11	$\rightarrow 50$	1.85E+11	$\rightarrow 168$	1.22E+11	$\rightarrow 49$	1.78E+12
352	8.63E+11	$\rightarrow 50$	4.82E+11	$\rightarrow 168$	2.31E+11	$\rightarrow 48$	1.14E+11	$\rightarrow 167$	6.42E+10	$\rightarrow 40$	1.78E+12
353	4.63E+11	$\rightarrow 52$	4.21E+11	$\rightarrow 51$	2.71E+11	$\rightarrow 170$	2.61E+11	$\rightarrow 169$	7.82E+10	$\rightarrow 55$	1.79E+12
354	2.48E+12	$\rightarrow 9$	5.70E+11	$\rightarrow 44$	3.30E+11	$\rightarrow 8$	2.58E+11	$\rightarrow 166$	2.23E+11	$\rightarrow 10$	4.51E+12
355	1.19E+12	$\rightarrow 48$	6.03E+11	$\rightarrow 167$	1.33E+08	$\rightarrow 155$	3.56E+07	$\rightarrow 33$	2.09E+07	$\rightarrow 343$	1.79E+12
356	6.91E+11	$\rightarrow 54$	4.95E+11	$\rightarrow 172$	1.40E+11	$\rightarrow 49$	1.36E+11	$\rightarrow 56$	8.49E+10	$\rightarrow 174$	1.76E+12
357	6.22E+11	$\rightarrow 52$	3.44E+11	$\rightarrow 53$	3.35E+11	$\rightarrow 170$	1.82E+11	$\rightarrow 171$	1.23E+11	$\rightarrow 51$	1.80E+12
358	9.14E+11	$\rightarrow 53$	4.72E+11	$\rightarrow 171$	2.59E+11	$\rightarrow 52$	1.33E+11	$\rightarrow 170$	4.14E+09	$\rightarrow 19$	1.81E+12
359	7.54E+11	$\rightarrow 175$	1.01E+11	$\rightarrow 178$	1.00E+11	$\rightarrow 176$	5.03E+10	$\rightarrow 182$	3.29E+09	$\rightarrow 179$	1.01E+12
360	9.46E+11	$\rightarrow 56$	5.83E+11	$\rightarrow 174$	8.66E+10	$\rightarrow 40$	1.08E+10	$\rightarrow 148$	9.57E+09	$\rightarrow 66$	1.65E+12
361	5.74E+11	$\rightarrow 55$	3.96E+11	$\rightarrow 173$	2.23E+11	$\rightarrow 54$	1.61E+11	$\rightarrow 172$	1.13E+11	$\rightarrow 47$	1.78E+12
362	7.22E+11	$\rightarrow 177$	2.26E+11	$\rightarrow 175$	5.15E+10	$\rightarrow 183$	1.01E+10	$\rightarrow 176$	1.40E+09	$\rightarrow 182$	1.02E+12
363	8.78E+11	$\rightarrow 176$	1.15E+11	$\rightarrow 179$	1.54E+10	$\rightarrow 182$	1.27E+09	$\rightarrow 162$	8.57E+08	$\rightarrow 50$	1.01E+12
364	7.95E+11	$\rightarrow 178$	1.14E+11	$\rightarrow 176$	6.33E+10	$\rightarrow 175$	3.67E+10	$\rightarrow 182$	3.01E+09	$\rightarrow 179$	1.02E+12
365	9.76E+11	$\rightarrow 182$	1.22E+10	$\rightarrow 176$	2.96E+09	$\rightarrow 179$	1.14E+09	$\rightarrow 56$	9.68E+08	$\rightarrow 162$	9.94E+11
366	6.46E+11	$\rightarrow 181$	2.83E+11	$\rightarrow 177$	5.12E+10	$\rightarrow 185$	2.30E+10	$\rightarrow 175$	6.37E+09	$\rightarrow 183$	1.02E+12
367	9.95E+11	$\rightarrow 179$	1.33E+09	$\rightarrow 48$	1.34E+08	$\rightarrow 167$	9.22E+05	$\rightarrow 33$	6.89E+04	$\rightarrow 355$	9.97E+11
368	7.78E+11	$\rightarrow 183$	1.69E+11	$\rightarrow 178$	3.25E+10	$\rightarrow 175$	2.07E+10	$\rightarrow 177$	7.52E+09	$\rightarrow 176$	1.02E+12
369	6.49E+11	$\rightarrow 184$	2.99E+11	$\rightarrow 181$	2.76E+10	$\rightarrow 177$	2.59E+10	$\rightarrow 185$	8.26E+09	$\rightarrow 183$	1.01E+12
370	7.92E+11	$\rightarrow 185$	1.75E+11	$\rightarrow 183$	1.96E+10	$\rightarrow 181$	8.70E+09	$\rightarrow 178$	7.84E+09	$\rightarrow 177$	1.01E+12
371	6.82E+11	$\rightarrow 59$	3.99E+11	$\rightarrow 180$	2.44E+11	$\rightarrow 55$	1.67E+11	$\rightarrow 173$	6.36E+10	$\rightarrow 47$	1.75E+12
372	3.27E+11	$\rightarrow 2$	1.36E+11	$\rightarrow 1$	1.30E+11	$\rightarrow 18$	8.31E+10	$\rightarrow 128$	6.59E+10	$\rightarrow 267$	8.97E+11
373	2.44E+11	$\rightarrow 16$	9.94E+10	$\rightarrow 126$	5.51E+10	$\rightarrow 260$	4.22E+10	$\rightarrow 20$	3.56E+10	$\rightarrow 129$	5.61E+11
374	2.38E+11	$\rightarrow 16$	9.60E+10	$\rightarrow 126$	5.19E+10	$\rightarrow 260$	3.64E+10	$\rightarrow 21$	3.08E+10	$\rightarrow 130$	5.35E+11
375	1.38E+12	$\rightarrow 1$	4.00E+11	$\rightarrow 17$	2.77E+11	$\rightarrow 2$	1.70E+11	$\rightarrow 127$	8.21E+10	$\rightarrow 266$	2.48E+12
376	1.66E+12	$\rightarrow 2$	4.73E+11	$\rightarrow 18$	2.04E+11	$\rightarrow 128$	9.97E+10	$\rightarrow 267$	1.18E+10	$\rightarrow 27$	2.47E+12
377	5.23E+11	$\rightarrow 20$	2.96E+11	$\rightarrow 129$	1.50E+11	$\rightarrow 270$	3.71E+10	$\rightarrow 21$	2.11E+10	$\rightarrow 130$	1.05E+12
378	5.58E+11	$\rightarrow 21$	3.16E+11	$\rightarrow 130$	1.62E+11	$\rightarrow 272$	4.31E+09	$\rightarrow 60$	3.15E+09	$\rightarrow 2$	1.05E+12
379	3.56E+11	$\rightarrow 279$	1.57E+10	$\rightarrow 201$	8.08E+09	$\rightarrow 280$	3.56E+08	$\rightarrow 202$	3.22E+08	$\rightarrow 131$	3.81E+11
380	3.17E+11	$\rightarrow 131$	2.39E+11	$\rightarrow 277$	1.17E+10	$\rightarrow 132$	8.84E+09	$\rightarrow 278$	5.60E+09	$\rightarrow 67$	5.89E+11
381	3.64E+11	$\rightarrow 280$	1.60E+10	$\rightarrow 202$	3.42E+08	$\rightarrow 132$	2.65E+07	$\rightarrow 278$	1.46E+07	$\rightarrow 114$	3.80E+11
382	3.28E+11	$\rightarrow 132$	2.48E+11	$\rightarrow 278$	5.69E+09	$\rightarrow 66$	5.33E+09	$\rightarrow 195$	9.55E+08	$\rightarrow 21$	5.88E+11
383	1.53E+11	$\rightarrow 9$	1.48E+11	$\rightarrow 61$	1.48E+11	$\rightarrow 6$	1.38E+11	$\rightarrow 10$	8.07E+10	$\rightarrow 191$	1.06E+12
384	2.29E+11	$\rightarrow 10$	1.49E+11	$\rightarrow 60$	1.05E+11	$\rightarrow 190$	9.73E+10	$\rightarrow 7$	7.71E+10	$\rightarrow 58$	1.01E+12
385	3.68E+11	$\rightarrow 2$	1.84E+11	$\rightarrow 46$	1.80E+11	$\rightarrow 45$	1.15E+11	$\rightarrow 1$	8.40E+10	$\rightarrow 187$	1.21E+12
386	4.92E+11	$\rightarrow 2$	2.10E+11	$\rightarrow 46$	1.46E+11	$\rightarrow 45$	1.41E+11	$\rightarrow 1$	9.51E+10	$\rightarrow 187$	1.36E+12
387	6.02E+11	$\rightarrow 2$	3.36E+11	$\rightarrow 46$	1.54E+11	$\rightarrow 187$	4.97E+10	$\rightarrow 195$	4.57E+10	$\rightarrow 66$	1.31E+12
388	3.92E+11	$\rightarrow 2$	1.94E+11	$\rightarrow 45$	1.67E+11	$\rightarrow 1$	1.60E+11	$\rightarrow 46$	7.97E+10	$\rightarrow 186$	1.26E+12
389	2.89E+11	$\rightarrow 2$	2.36E+11	$\rightarrow 1$	2.13E+11	$\rightarrow 45$	1.17E+11	$\rightarrow 46$	8.63E+10	$\rightarrow 186$	1.23E+12
390	1.31E+12	$\rightarrow 8$	1.18E+12	$\rightarrow 9$	5.84E+11	$\rightarrow 6$	4.41E+11	$\rightarrow 57$	4.33E+11	$\rightarrow 10$	4.77E+12
391	1.85E+12	$\rightarrow 6$	6.28E+11	$\rightarrow 58$	2.76E+11	$\rightarrow 188$	1.91E+11	$\rightarrow 7$	1.22E+11	$\rightarrow 60$	3.38E+12
392	1.30E+12	$\rightarrow 7$	7.90E+11	$\rightarrow 60$	3.32E+11	$\rightarrow 190$	2.13E+10	$\rightarrow 272$	1.51E+10	$\rightarrow 80$	2.53E+12
393	3.28E+12	$\rightarrow 10$	6.44E+11	$\rightarrow 61$	2.80E+11	$\rightarrow 191$	1.58E+11	$\rightarrow 7$	1.26E+11	$\rightarrow 6$	4.80E+12
394	2.08E+12	$\rightarrow 8$	5.26E+11	$\rightarrow 10$	3.68E+11	$\rightarrow 57$	1.76E+11	$\rightarrow 189$	1.75E+11	$\rightarrow 62$	3.98E+12
395	1.47E+12	$\rightarrow 10$	1.14E+12	$\rightarrow 9$	2.99E+11	$\rightarrow 63$	2.05E+11	$\rightarrow 192$	2.04E+11	$\rightarrow 61$	3.97E+12
396	9.01E+11	$\rightarrow 69$	5.07E+11	$\rightarrow 193$	1.50E+11	$\rightarrow 67$	8.69E+10	$\rightarrow 194$	3.96E+10	$\rightarrow 71$	1.79E+12
397	9.51E+11	$\rightarrow 71$	5.26E+11	$\rightarrow 196$	1.31E+11	$\rightarrow 66$	6.95E+10	$\rightarrow 195$	1.95E+10	$\rightarrow 54$	1.79E+12
398	9.14E+11	$\rightarrow 199$	6.29E+10	$\rightarrow 201$	3.88E+10	$\rightarrow 200$	1.74E+10	$\rightarrow 279$	1.91E+09	$\rightarrow 202$	1.04E+12
399	9.85E+11	$\rightarrow 67$	5.37E+11	$\rightarrow 194$	3.50E+10	$\rightarrow 66$	3.41E+10	$\rightarrow 277$	3.35E+10	$\rightarrow 196$	1.76E+12
400	9.46E+11	$\rightarrow 200$	6.80E+10	$\rightarrow 202$	1.72E+10	$\rightarrow 280$	2.35E+09	$\rightarrow 201$	1.07E+09	$\rightarrow 71$	1.04E+12
401	1.08E+12	$\rightarrow 66$	5.91E+11	$\rightarrow 195$	3.51E+10	$\rightarrow 278$	2.29E+10	$\rightarrow 56$	1.94E+10	$\rightarrow 100$	1.77E+12
402	7.11E+11	$\rightarrow 73$	4.24E+11	$\rightarrow 197$	1.68E+11	$\rightarrow 69$	1.37E+11	$\rightarrow 74$	8.93E+10	$\rightarrow 193$	1.82E+12
403	7.85E+11	$\rightarrow 74$	5.08E+11	$\rightarrow 198$	1.72E+11	$\rightarrow 71$	1.58E+11	$\rightarrow 75$	8.79E+10	$\rightarrow 196$	1.81E+12
404	9.48E+11	$\rightarrow 201$	5.29E+10	$\rightarrow 279$	1.98E+10	$\rightarrow 202$	1.42E+09	$\rightarrow 280$	1.10E+09	$\rightarrow 67$	1.02E+12
405	9.67E+11	$\rightarrow 202$	5.42E+10	$\rightarrow 280$	1.22E+09	$\rightarrow 66$	6.71E+08	$\rightarrow 114$	1.85E+08	$\rightarrow 271$	1.02E+12
406	8.66E+11	$\rightarrow 203$	8.34E+10	$\rightarrow 199$	6.06E+10	$\rightarrow 204$	2.07E+10	$\rightarrow 279$	4.23E+09	$\rightarrow 200$	1.04E+12
407	9.28E+11	$\rightarrow 204$	8.11E+10	$\rightarrow 200$	2.02E+10	$\rightarrow 280$	3.93E+09	$\rightarrow 199$	2.07E+09	$\rightarrow 124$	1.04E+12