Atomic data from the IRON project - LXVIII. Electron impact excitation of Fe xi

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Table 3:

List of energies (cm^-1) for the lowest 48 levels of Fe XI.
i	Conf.	Lev.	$E_{\rm exp}$	$E_{\rm target}$	$E_{\rm bench}$	$E_{\rm bench}$ (TEC)	$E_{\rm MR-MP}$	$E_{\rm NIST}$
1	3s² 3p⁴	³P $_{2}^{\rm e}$	0	0	0	0	0	0
2	3s² 3p⁴	³P $_{1}^{\rm e}$	12 667	12 587 (80)	12 371 (297)	12 397 (271)	12 667 (0)	12 667 (0)
3	3s² 3p⁴	³P $_{0}^{\rm e}$	14 306	14 245 (61)	14 283 (23)	14 155 (151)	14 312 (-6)	14 312 (-6)
4	3s² 3p⁴	¹D $_{2}^{\rm e}$	37 743	39 504 (-1761)	38 324 (-581)	37 748 (-5)	37 743 (-1)	37 743 (-1)
5	3s² 3p⁴	¹S $_{0}^{\rm e}$	80 831	80 190 (641)	83 640 (-2809)	80 842 (-11)	80 814 (16)	80 814 (16)
6	3s 3p⁵	³P $_{2}^{\rm o}$	283 551	279 487 (4064)	283 764 (-213)	283 658 (-107)	283 739 (-188)	283 558 (-7)
7	3s 3p⁵	³P $_{1}^{\rm o}$	293 158	289 178 (3980)	293 229 (-71)	293 089 (69)	293 315 (-157)	293 158 (0)
8	3s 3p⁵	³P $_{0}^{\rm o}$	299 163	295 116 (4047)	299 059 (104)	298 953 (210)	299 308 (-145)	299 163 (0)
9	3s 3p⁵	¹P $_{1}^{\rm o}$	361 846	362 521 (-675)	365 012 (-3166)	361 678 (168)	361 675 (171)	361 842 (4)
10	3s² 3p³ 3d	⁵D $_{0}^{\rm o}$	387 544	386 037 (1507)	389 671 (-2127)	387 427 (117)	387 622 (-78)	-
11	3s² 3p³ 3d	⁵D $_{1}^{\rm o}$	387 726	386 278 (1448)	389 870 (-2144)	387 628 (98)	387 811 (-85)	-
12	3s² 3p³ 3d	⁵D $_{2}^{\rm o}$	387 940	386 584 (1356)	390 118 (-2178)	387 866 (74)	388 020 (-80)	-
13	3s² 3p³ 3d	⁵D $_{3}^{\rm o}$	388 268	387 049 (1219)	390 506 (-2238)	388 236 (32)	388 335 (-67)	-
14	3s² 3p³ 3d	⁵D $_{4}^{\rm o}$	389 227	388 180 (1047)	391 510 (-2283)	389 244 (-17)	389 274 (-47)	-
15	3s² 3p³ 3d	³D $_{2}^{\rm o}$	412 856	413 327 (-471)	416 494 (-3638)	413 082 (-226)	412 968 (-112)	-
16	3s² 3p³ 3d	³D $_{3}^{\rm o}$	415 426	415 958 (-532)	418 774 (-3348)	415 618 (-192)	415 477 (-51)	-
17	3s² 3p³ 3d	³D $_{1}^{\rm o}$	417 049	417 529 (-480)	420 300 (-3251)	417 205 (-156)	417 139 (-90)	-
18	3s² 3p³ 3d	³F $_{2}^{\rm o}$	422 844	423 871 (-1027)	426 701 (-3857)	422 557 (287)	422 920 (-76)	-
19	3s² 3p³ 3d	¹S $_{0}^{\rm o}$	-	426 304	428 625	425 466	425 465	-
20	3s² 3p³ 3d	³F $_{3}^{\rm o}$	426 022	427 435 (-1413)	429 980 (-3958)	425 712 (310)	426 149 (-127)	-
21	3s² 3p³ 3d	³F $_{4}^{\rm o}$	430 522	432 267 (-1745)	434 444 (-3922)	430 102 (420)	430 589 (-67)	-
22	3s² 3p³ 3d	³G $_{3}^{\rm o}$	-	452 321	453 512	448 623	448 615	-
23	3s² 3p³ 3d	³G $_{4}^{\rm o}$	450 211	454 113 (-3902)	455 092 (-4881)	450 218 (-7)	450 228 (-17)	-
24	3s² 3p³ 3d	³G $_{5}^{\rm o}$	452 416	456 642 (-4226)	457 218 (-4802)	452 414 (2)	452 413 (3)	-
25	3s² 3p³ 3d	¹G $_{4}^{\rm o}$	459 218	463 779 (-4561)	464 621 (-5403)	459 220 (-2)	459 231 (-13)	-
26	3s² 3p³ 3d	¹D $_{2}^{\rm o}$	-	468 495	472 489	466 545	466 458	-
27	3s² 3p³ 3d	³D $_{1}^{\rm o}$	-	484 112	488 110	481 678	481 722	-
28	3s² 3p³ 3d	³P $_{0}^{\rm o}$	-	484 177	488 573	482 071	482 618	-
29	3s² 3p³ 3d	³P $_{1}^{\rm o}$	484 830	486 900 (-2070)	491 259 (-6429)	484 676 (154)	484 990 (-160)	-
30	3s² 3p³ 3d	³F $_{3}^{\rm o}$	485 039	488 474 (-3435)	491 500 (-6461)	485 125 (-86)	485 081 (-42)	-
31	3s² 3p³ 3d	³F $_{2}^{\rm o}$	-	489 360	492 645	486 234	486 227	-
32	3s² 3p³ 3d	³F $_{4}^{\rm o}$	486 413	490 069 (-3656)	492 671 (-6258)	486 445 (-32)	486 412 (1)	-
33	3s² 3p³ 3d	³D $_{2}^{\rm o}$	489 378	492 380 (-3002)	495 788 (-6410)	489 376 (2)	489 528 (-150)	-
34	3s² 3p³ 3d	³P $_{2}^{\rm o}$	494 013	496 544 (-2531)	500 566 (-6553)	494 055 (-42)	494 053 (-40)	496 090 (-2077)
35	3s² 3p³ 3d	³D $_{3}^{\rm o}$	497 235	500 555 (-3320)	503 664 (-6429)	497 216 (19)	497 452 (-217)	-
36	3s² 3p³ 3d	¹F $_{3}^{\rm o}$	525 260	530 347 (-5087)	532 842 (-7582)	525 278 (-18)	525 332 (-72)	-
37	3s² 3p³ 3d	³P $_{1}^{\rm o}$ $^{\dagger}$	531 070	536 811 (-5741)	540 265 (-9195)	530 770 (300)	531 839 (-769)	526 480 (4590)
38	3s² 3p³ 3d	³P $_{2}^{\rm o}$	531 304	537 000 (-5696)	541 300 (-9996)	531 551 (-247)	531 502 (-198)	531 290 (14)
39	3s² 3p³ 3d	³S $_{1}^{\rm o}$ $^{\dagger}$	533 445	540 191 (-6746)	543 921 (-10 476)	533 838 (-393)	533 343 (102)	533 450 (-5)
40	3s² 3p³ 3d	³P $_{0}^{\rm o}$	541 777	547 599 (-5822)	551 873 (-10 096)	542 143 (-366)	541 892 (-115)	541 720 (57)
41	3s² 3p³ 3d	³P $_{1}^{\rm o}$ $^{\dagger}$	541 424	547 732 (-6308)	551 800 (-10 376)	541 729 (-305)	541 178 (246)	541 390 (34)
42	3s² 3p³ 3d	³D $_{3}^{\rm o}$	554 321	561 699 (-7378)	564 972 (-10 651)	554 308 (13)	554 305 (16)	554 300 (21)
43	3s² 3p³ 3d	³D $_{2}^{\rm o}$	561 615	569 308 (-7693)	572 350 (-10 735)	561 671 (-56)	561 556 (59)	561 610 (5)
44	3s² 3p³ 3d	³D $_{1}^{\rm o}$	566 396	573 992 (-7596)	577 055 (-10 659)	566 321 (75)	566 299 (97)	566 380 (16)
45	3s² 3p³ 3d	¹D $_{2}^{\rm o}$	578 890	587 776 (-8886)	589 847 (-10 957)	578 887 (3)	578 539 (351)	578 860 (30)
46	3s² 3p³ 3d	¹F $_{3}^{\rm o}$	594 047	603 720 (-9673)	605 953 (-11 906)	594 047 (0)	594 518 (-471)	594 030 (17)
47	3s² 3p³ 3d	¹P $_{1}^{\rm o}$	623 101	631 099 (-7998)	636 559 (-13 458)	623 094 (7)	623 252 (-151)	623 080 (21)
48	3p⁶	¹S $_{0}^{\rm e}$	-	638 441	625 608	614 643	-	-

Notes. $^{(\dagger)}$ Lower, middle and upper J=1.
The experimental level energies $E_{\rm exp}$ (Del Zanna 2010) are shown, together with those obtained from our scattering target $E_{\rm target}$ , those from our benchmark $E_{\rm bench}$ , those from our benchmark including TEC $E_{\rm bench}$ (TEC). We also list the values from the NIST compilation ( $E_{\rm NIST}$ ) and those calculated with the many-body perturbation theory ( $E_{\rm MR-MP}$ ) by Ishikawa & Vilkas (2008). Values in parentheses indicate differences with $E_{\rm exp}$ .

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