Extended analysis of spectra and term systems in aluminumlike Ca viii–Ni xvi

Andreas Redfors; Ulf Litzén

doi:10.1364/JOSAB.6.001447

Journal of the Optical Society of America B
Vol. 6,
Issue 8,
pp. 1447-1456
(1989)
•https://doi.org/10.1364/JOSAB.6.001447

Extended analysis of spectra and term systems in aluminumlike Ca viii–Ni xvi

Andreas Redfors and Ulf Litzén

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
Andreas Redfors and Ulf Litzén, "Extended analysis of spectra and term systems in aluminumlike Ca viii–Ni xvi," J. Opt. Soc. Am. B 6, 1447-1456 (1989)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Abstract

Spectra emitted from laser-produced plasmas of Ca, Sc, Ti, V, Cr, Mn, Fe, Co, and Ni have been recorded in the region 170–800 Å. In aluminumlike Ca viii–Ni xvi, transitions establishing all terms in the configurations 3s²3p, 3s3p², 3s²3d, 3p³, and 3s3p3d (except ⁴F) have been identified, and new and improved level values have been derived. Ab initio and parametric calculations support the identifications and provide eigenvector components.

Full Article | PDF Article

More Like This

Extended analysis of spectra and 3l4l^′ energy levels in Mg-like Sc x–Fe xv

Ilmar Kink, Magnus Tunklev, and Ulf Litzén
J. Opt. Soc. Am. B 14(4) 722-730 (1997)

Analysis of magnesiumlike spectra from Cu xviii to Mo xxxi

J. Sugar, V. Kaufman, P. Indelicato, and W. L. Rowan
J. Opt. Soc. Am. B 6(8) 1437-1443 (1989)

Chlorinelike spectra of copper to molybdenum

Victor Kaufman, Jack Sugar, and William L. Rowan
J. Opt. Soc. Am. B 6(8) 1444-1446 (1989)

Previous Article Next Article

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (5)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (5)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

		Ca viii		Sc ix		Ti x		V xi		Cr xii		Mn xiii		Fe xiv		Co xv		Ni xvi

Transition		λ(Å)^b	Int.	λ(Å)^b	Int.	λ(Å)^b	Int.	λ(Å)^b	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.
3s²3p²P_3/2–3s3p²	²D_3/2	597.855	3	538.075	2	488.971	1	447.881	1	–		–		–		–		–
²P_3/2	²D_5/2	596.935	9	536.982	7	487.654	4	446.265	6	410.989	4p	380.501	6	353.829	6	330.247	5	309.196	5
²P_1/2	²D_3/2	582.845	8	521.894	5	471.574	3	429.232	4	393.028	3	361.659	5	334.171	5	309.849	5bl	288.149	4
²P_1/2	²S_1/2	471.085	m	426.256	4	389.237	2	358.144	3	331.687	3	308.920^c	–	289.123	1	–		–
²P_1/2	²S_1/2	461.711	8	416.041	6	378.135	4	346.123	5	318.722	4	294.985	6	274.203	6	255.852	8bl	239.510	5
²P_3/2	²P_1/2	441.089	8	399.888	7	365.628	5	336.580	6	311.587	5	289.774	6	270.511	6	253.326	5p	237.859	4
²P_3/2	²P_3/2	436.141	10	394.647	8	360.133	7	330.913	8	305.816	8p	283.984	8	264.785	7	247.740	6	232.483	9p
²P_1/2	²P_1/2	432.869	9	390.888	6	355.815	5	325.945	6	300.120	4p	277.469	4	257.377	3p	239.376	6bl	223.117	1
²P_1/2	²P_3/2	428.094	8	385.869	4	350.610	4	320.626	3	294.758	3	272.154	4	252.188	3	234.385	3	218.383	2
3s²3p²P_3/2–3s²3d	²D_3/2	359.660	5	324.568	6bl	296.040	2	272.332	2	252.276	1	235.054	4bl	220.076	1p	206.924	1p	195.266c	–
²P_3/2–	²D_5/2	359.369	8	324.195	7	295.556	5p	271.773	8	251.578	5	234.235	6	219.136	4	205.848	4	194.049	4
²P_1/2–	²D_3/2	354.168	7	318.606	5	289.576	4p	265.324	6	244.708	3	226.905	5	211.331	2	197.554	3	185.251	1

		Ca viii		Sc ix		Ti x		V xi		Cr xii		Mn xiii		Fe xiv		Co xv		Ni xvi

Transition		λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.	λ(Å)	Int.
3s3P²P_3/2–	3P^3 2P_1/2	696.802	1	–		–		–		–		–		–		–		–
²P_3/2–	²P_3/2	696.133	1	623.088	0	563.358	1	513.315	2	470.868	1	–		–		–		–
²P_1/2–	²P_1/2	684.482	1	611.704	0	552.090	1	502.602	1	460.775	0	425.038	1	–		–		–
²D_3/2–	²D_3/2	608.733	4	547.190	2	496.647	1	454.325	1	418.406	2	387.585	3	(360.827)	m	337.422	3	316.811	3p
²D_5/2–	²D_5/2	607.979	4	546.332	2	495.671	2	453.162	3	417.006	3	385.827	4	358.681	4	334.852	4	313.724	4
²D_5/2–	²P_3/2	486.824	6	439.299	4bl	399.797^b	bl	366.403	3p	337.772	3	312.802	3h	290.747	2p	271.126	2p	–
²D_3/2–	²P_1/2	486.527	5	439.128	4bl	399.797^b	bl	366.579	2p	338.116	2p	313.337	6bl	291.492	3p	272.159	2	–
²D_3/2–	²P_3/2	486.218	2	–		–		–		–		–		–		–		–
⁴P_5/2	⁴S_3/2^c	471.183	8	426.855	6	390.016	4	358.846	6	332.126	5	308.895	7	288.512	6	270.378	5	254.139	3
⁴P_3/2–	⁴S_3/2^c	465.993	7	421.231	5	383.913	3p	352.334	5	325.177	4	301.525	5	280.739	4	262.249	3	245.671	2
⁴P_1/2–	⁴S_3/2^c	462.591	6	417.462	4	379.780	2	347.787	4	320.191	3	296.073	3	274.797	2	255.828	8bl	238.699	1
3s²3.d²D_3/2–3s3p(³P)3d	²F_5/2	618.466	2bl	–		–		–		–		–		–		–		–
²D_5/2–	²F_7/2	606.450	2	–		–		–		–		–		–		–		–
3s²3d²D_5/2–3s3p(¹P)3d	²F_7/2	491.098	7	441.743	5	401.347	3	367.516	3	338.689	5	313.801	5	292.036	3	272.855	7	255.741	5
D_3/2–	²F_5/2	488.452	6	438.851	4	398.174	3	364.073	2	335.017	4	309.857	3	287.859	3	268.424	4	251.088	3
²D_5/2–	²D_3/2	–		–		–		–		–		293.581	5	273.538	2	(255.762)	m	239.904	2
²D_5/2–	²P_3/2	455.366	7bl	410.840	4bl	374.031	2bl	342.982	4bl	316.466	5bl	–		–		–		–
²D_3/2–	²P_1/2	455.366	7bl	410.840	4bl	374.031	2bl	342.982	4bl	316.466	5bl	293.268	3bl	273.000	2	255.113	3	239.055	1
²D_3/2~	²D_3/2	446.990	5	404.500	2	369.038	2	338.971	2	312.949	4bl	290.114	4	269.926	2	251.949	2	235.776	1
²D_5/2–	²D_5/2	446.250	6	403.853	4	368.564	3	338.681	3	312.949	4bl	290.539	5	270.765	2	253.239	4p	237.470	4p
²D_3/2–	²D_5/2	445.789	2p	–		–		–		–		–		–		–		–
3s3p^2 2D_5/2–3s3p(³P)3d	²D_5/2	397.171	8	358.175	6	326.258	4	299.548	5	276.818	4	257.234	8bl	240.159	4	225.083	3	211.715	3
²D_3/2–	²D_3/2	396.755	7	(357.722)	m	325.743	3	298.960	4	276.191	2	256.497	4	239.231	2	(223.992)	m	210.375	2
²S_1/2–	²P_3/2	(374.100)	m	336.922	3	306.758	2	281.668	3	260.429	3	242.066	3	226.040	1	211.879	1p	199.210	2
²S_1/2–	²P_1/2	372.153	3	334.681	2	304.233	1	278.824	1p	–		–		–		–		–
²D_5/2–	²F_5/2	367.337	4	–		–		–		–		–		–		–		–
²D_3/2–	²F_5/2	367.000	6p	331.186	4p	302.024	2bl	277.778	2bl	257.282	2p	239.680	2	224.354	1	210.861	2	198.844	1
²D_5/2–	²F_7/2	362.779	6	326.642	4	297.138	3	272.568	3	251.744	3p	233.767	7bl	218.169	2	204.394	3	192.187	3
⁴P_5/2–	⁴P_5/2	363.387	4	327.980	2	299.223	1h	–		–		–		–		–		–
⁴P_5/2–	⁴P_3/2	361.999	4	–		297.972	1h	–		–		–		–		–		–
⁴P_3/2	⁴P_5/2	360.285	6	324.641	6bl	(295.617)	m	271.572	2p	251.223	3	233.767	7bl	218.578	2	205.229	2	193.412	2p
⁴P_1/2–	⁴P_3/2	356.906	5	321.111	4	291.938	2	267.658	3	247.065	2	–		–		–		–
⁴P_3/2–	⁴P_1/2	–		–		–		267.249	1	246.255	2p	228.264	1	–		–		–
⁴P_1/2–	⁴P_1/2	356.225	4	320.116	2	290.959	2h	–		–		–		–		–		–
⁴P_3/2–	⁴P_3/2	–		–		–		–		–		227.445	3h	–		–		–
⁴P_5/2–	⁴D_3/2	357.961	3	322.751	2	293.956	1	–		–		–		–		–		–
⁴P_5/2–	⁴D_5/2	357.487	7	322.321	7bl	(293.700)	m	269.718	4	249.374	2p	231.868	4	216.576	1p	203.086	3p	191.055	1
⁴P_5/2–	⁴D_7/2	357.333	9	322.321	7p	293.665	4p	269.828	6	249.572	3	232.158	5	216.928	2	203.468	3	191.486	3
⁴P_3/2–	⁴D_1/2	355.685	6	320.451	1p	291.379	1	–		–		–		–		–		–
⁴P_3/2–	⁴D_3/2	354.963	6	319.568	4bl	290.528	2	266.202	2	245.469	2bl	–		–		–		–
⁴P_1/2–	⁴D_3/2	–		–		–		–		–		229.355	3	213.906	1p	–		–
⁴P_3/2–	⁴D_5/2	354.452	7bl	319.115	3	290.226	2bl	265.988	2bl	245.469	2p	227.704	4	212.154	1	198.451	1	–
⁴P_1/2–	⁴D_1/2	353.674	4	–				266.675	4h	246.200	2	228.500	1p	213.176	1	199.558	1	187.404	1
3s3p^2 2P_3/2–3s3p(¹P)3d	²P_1/2	372.619	3	335.495	1	–		–		–		–		–		–		–
²P_3/2–	²P_3/2	372.279	5p	–		304.867	1	279.778	3h	–		239.255	3	223.618	1	209.873	2p	(197.614)	m
²P_1/2–	²P_1/2	369.053	4	331.792	2p	–		276.541	1	255.456	1	237.369	1	–		–		–
²P_1/2–	²P_3/2	368.763	6	331.318	2p	301.028	1p	275.869	3p	254.768	2	(235.292)	m	–		–		–
²P_3/2–	²D_3/2	367.000	6p	331.186	4p	302.024	2bl	277.778	2bl	257.112	2	–		–		–		–
²P_3/2–	²D_5/2	366.191	6p	330.399	5	301.254	3	276.963	4	256.370	5bl	238.675	5	223.222	2	209.620	3	197.515	2p
²P_1/2–	²D_3/2	363.547	5	327.618	3	298.303	2	273.888	3	253.168	2	236.723	5	221.124	1	207.458	3	195.391	1p
²D_5/2–	²F_7/2	318.073	5	286.887	5bl	261.494	1	240.333	2p	222.491	1	207.130	3	–		–		–
²D_5/2–	²F_5/2	317.206	2	–		–		–		–		–		–		–		–
²D_3/2–	²F_5/2	316.928	5	285.610	3	260.142	1	238.892	2	220.890	1	205.350	2	–		–		–

Energy Level		Ca viii	Sc ix	Ti x	V xi	Cr xii	Mn xiii	Fe xiv	Co xv	Ni xvi
3s²3p	²P_1/2	0	0	0	0	0	0	0	0	0
	²P_3/2^b	4 308	5 761	7 543	9 696	12 261	15 295	18 852	22 984	27 756
3s3p²	⁴P_1/2^c	129 772	144 954	160 381	176 101	192 115	208 443	225 095	242 133	259 489
	⁴P_3/2^c	131 350	147 076	163 216	179 812	196 904	214 550	232 805	251 704	271 370
	⁴P_5/2^c	133 714	150 233	167 292	184 963	203 338	222 463	242 401	263 175	284 949
	²D_3/2	171 572	191 610	212 055	232 972	254 435	276 504	299 247	322 738	347 043
	²D_5/2	171 830	191 987	212 606	233 778	255 577	278 106	301 474	325 788	351175
	²S_1/2	216 585	240 361	264 456	288 914	313 752	339 000	364 697	390 851	417 519
	²P_1/2	231 018	255 829	281 045	306 801	333 199	360 396	388 529	417 743	448 184
	²P_3/2	233 593	259 154	285 218	311 890	339 258	367 434	396 524	426 641	457 903
3s²3d	²D_3/2	282 350	313 865	345 334	376 897	408 651	440 721	473 191	506 191	539 808
	²D_5/2	282 574	314 217	345 888	377 650	409 752	442 217	475 190	508 779	543 090
3 p³	²D_3/2	335 848	374 362	413 405	453 079	493 437	534 512	576 388^d	619 102	662 689
	²D_5/2	336 309	375 026	414 353	454 450	495 382	537 290	580 273	624 427	669 927
	⁴S_3/2	345 946	384 492	423 692	463 634	504 429	546 198	589 005	633 024	678 426
	²P_1/2	377 110	419 307	462 175	505 765	550 208	595 669	642 310	690 170
	²P_3/2	377 243	419 645	462 725	506 702	551 634	597 797	645 416	694 620
3s3p(³P)3d	⁴P_5/2	408 906	455 130	501 491	548 039	594 957	642 326	690 308	738 965	788 401
	⁴P_3/2	409 958	456 373	502 907	549 712	596 867	654 217
	⁴P_1/2	410 493	457 341	504 072	553 995	602 987	652 639
	⁴D_3/2	412 508	459 136	506 412	551 089	598 289	646 080	694 191	743 240	793 096
	⁴D_3/2	413 072	460 069	507 450	555 467	604 287^e	644 448	692 590
	⁴D_5/2	413 444	460 443	507 775	555 721	604 342	653 730	704 147	755 592	808 358
	⁴D_7/2	413 565	460 483^e	507 816^e	555 569	604 024	653 204	703 383	754 653	807 180
	²D_5/2	423 611	471 180	519 112	567 614	616 825	666 857^e	717 865	770 069	823 508
	²D_3/2	423 617	471 157^d	519 045	567 465	616 503	666 372	717 253	769 183^d	822 385
	²F_5/2	444 051	493 555^e	543 155^e	592 972	643 114	693 727	744 971	796 984	849 950
	²F_7/2	447 474	498 133	549 150	600 659	652 806	705 882	759 834	815 039	871 502
	²P_3/2	483 893^d	537 166	590 438	643 942	697 734	752 110	807 097	862 818	919 502
	²P_1/2	485 292	539 153	593 151	647 563
3s3p(¹P)3d	²F_7/2	486 212	540 593	595 037	649 747	705 021	760 893	817 614	875 274	934 111
	²F_5/2	487 087	541 736	596 470	651 570	707 146	763 464	820 583	878 736	938 075
	²P_1/2	501 976	557 221	612 692^e	668 411	724 656	781 681	839 491	898 174	958 122
	²P_3/2	502 195	557 654^e	613 235	669 304	725 713	785 399	843 689	903 110	963 939
	²D_3/2	506 078	561 073	616 292	671 911	728 194	782 835	840 767	899 768	959 923
	²D_5/2	506 670	561 825	617 188	672 931	729 319^e	786 410	844 512	903 680	964 196

Configuration	J	Percentage Composition in Ca viii, Sc ix, Ti x, V xi, Cr xii, Mn xiii, Fe xiv, Co xv and Ni xvi, Respectively^b
3s²3p	1/2	96, 96, 96, 96, 96, 97, 97, 97, 97% s²p²P; 2,2, 2, 2, 2, 2, 2, 2,1% p^3 2P
	3/2	96, 96, 96, 96, 96, 97, 97, 97, 97% s²p²P; 2, 2, 2, 2, 2, 2, 2, 2, 2% p^3 2P
3p³	3/2	65, 66, 66, 66, 66, 65, 64, 62, 59% p^{3 2}D; 33, 32, 32, 31, 30, 30, 29, 28, 27% sp(³P)d²D; 0, 0, 0, 0, 0, 1, 2, 3, 5% p^3 4S
	5/2	66, 67, 67, 67, 68, 68, 68, 68, 68% p^{3 2}D; 33, 32, 32, 31, 31, 31, 31, 31, 31% sp(³P)d²D
	3/2	98, 98, 97, 97, 96, 95, 93, 91, 88% p^{3 4}S; 0, 0, 1, 1, 2, 3, 4, 6, 8% p³; 1, 1, 1, 1, 1, 1, 1, 1, 1% pd²
	1/2	77, 78, 78, 79,79, 79, 80, 80, 80% p^{3 2}P; 20, 20, 19, 18, 18, 18, 18, 18, 18% spd
	3/2	76, 76, 75, 75, 74, 73, 72, 70, 68% p^{3 2}P; 20, 20, 20, 19, 19, 19, 20, 20, 21% spd; 0, 0, 1, 2, 2, 3, 4, 5, 6% p^3 4S
3s3p(³P)3d	3/2	100, 100, 99, 99, 99, 98, 98, 98, 98% sp(³P)d⁴F
	5/2	100, 100, 99, 99, 99, 99, 99, 98, 98% sp(³P)d⁴F
	7/2	100, 100, 99, 99, 99, 99, 99, 98, 98% sp(³P)d⁴F
	9/2	100, 100, 100, 100, 100, 100, 100, 100, 100% sp(³P)d⁴F
	5/2	91, 87, 83, 79, 75, 72, 69, 67, 65% sp(³P)d⁴P; 8, 11, 15, 18, 21, 24, 26, 27, 28% sp(³P)d⁴D
	3/2	86, 78, 69, 61, 53, 48, 43, 40, 38% sp(³P)d⁴P; 13, 21, 30, 38, 45, 51, 55, 57, 59% sp(³P)d⁴D
	1/2	89, 75, 53, 35, 25, 19, 15, 13, 12% sp(³P)d⁴P; 11, 25, 46, 64, 75, 80, 84, 86, 87% sp(³P)d⁴D
	1/2	89, 75, 53, 35, 25, 19, 15, 13, 12% sp(³P)d⁴D; 11, 25, 46, 64, 75, 80, 84, 86, 87% sp(³P)d⁴P
	3/2	86, 78, 69, 61, 54, 48, 44, 41, 39% sp(³P)d ⁴D; 13, 21, 30, 38, 45, 51, 55, 57,59% sp(³P)d⁴P
	5/2	91, 88, 84, 81, 78, 75, 73, 72, 71% sp(³P)d⁴D; 8, 11, 15, 18, 21, 23, 25, 26, 26% sp(³P)d⁴P
	7/2	99, 99, 99, 99, 99, 99, 98, 98, 98% sp(³P)d⁴D
	3/2	48, 48, 49, 49, 50, 50, 50, 49, 49% sp(³P)d²D; 32, 31, 30, 30, 29,29, 28, 28, 27% sp(¹P)d²D; 18, 18, 18, 18, 18, 18, 18, 18, 18% p^3 2D
	5/2	47, 48, 48, 49, 48, 48, 47, 47, 45% sp(³P)d²D) 32, 31, 30, 30, 29, 28, 27, 26, 25% sp(¹P)d²D; 18, 17, 17, 17, 17, 16, 16, 16, 16% p^3 2D
	5/2	64, 64, 64, 64, 64, 65, 65, 65, 65% sp(³P)d²F; 35, 35, 34, 34, 33, 33, 32, 32, 31% sp(¹P)d²F
	7/2	63, 63, 63, 64, 64, 65, 65, 66, 66% sp(³P)d²F; 36, 36, 35, 35, 35, 34, 34, 33, 33% sp(¹P)d²F
	3/2	82, 82, 81, 81, 80, 78, 77, 75, 73% sp(³P)d²P; 16, 16, 15, 15, 15, 15, 15, 15, 15% p^3 2P; 0, 0, 1, 2, 3, 4, 5, 7, 8% sp(¹P)d²D
	1/2	84, 85, 85, 85, 86, 86, 86, 86, 86% sp(³P)d²P; 15, 14, 14, 13, 13, 13, 12, 12, 12% p^3 2P
3s3p(¹P)3d	7/2	61, 61, 62, 62, 63, 63, 64, 64, 65% sp(¹P)d²F; 36, 36, 36, 35, 35, 34, 34, 33, 33% sp(³P)d²F
	5/2	62, 62, 63, 63, 64, 64, 64, 65, 65% sp(¹P)d²F; 35, 35, 35, 34, 34, 33, 33, 32, 31% sp(³P)d²F
	1/2	89, 89, 89, 90, 90, 90, 90, 90, 90% sp(¹P)d²P; 5, 4, 4,4, 4, 3, 3, 3, 3% pd²
	3/2	85, 82, 75, 60, 42, 29, 22, 18, 15% sp(¹P)d²P; 2, 5, 10, 21, 34, 43, 47, 49, 50% sp(¹P)d²D; 2, 4, 6, 9, 12, 16, 19, 20, 22% sp(³P)d
	3/2	61, 59, 53, 43, 30, 20, 15, 12, 10% sp(¹P)d²D; 3, 6, 14, 29, 47, 60, 68, 72, 74% sp(¹P)d²P; 17, 17, 16, 14, 12, 10, 8, 8, 8% sp(³P)d
	5/2	63, 64, 65, 65, 65, 65, 65, 65, 65% sp(¹P)d²D; 18, 18, 18, 18, 17, 17, 17, 17, 17% sp(³P)d²D; 14, 14, 14, 14, 13, 13, 13, 13, 13% p^3 2D

Configuration	J	Percentage Composition in Ca viii, Sc ix, Ti x, V xi, Cr xii, Mn xiii, Fe xiv, Co xv and Ni xvi, Respectively^b
3s3p²	1/2	99, 99, 99,99,99, 99,98, 98,98% sp^{2 4}P; 0, 0, 0, 0, 0, 0, 1, 1, 2% sp^2 2S
	3/2	99, 99, 99, 99, 99, 99, 99, 99, 99% sp^{2 4}P
	5/2	99, 99, 99, 99, 98, 98, 97, 97, 96% sp^{2 4}P; 0, 0, 0, 0, 1, 1, 2, 2, 3% sp^2 2D
	3/2	85, 85, 85, 86, 86, 86, 86, 86, 85% sp^{2 2}D; 13, 13, 12,12, 12, 12, 12, 12, 12% s²d²D
	5/2	85, 85, 85, 85, 85, 85, 85, 84, 84% sp^{2 2}D; 13, 13, 12, 12, 12, 12, 12, 11, 11% s²d²D; 0, 0, 0, 0, 1, 1, 2, 3, %%sp^2 4P
	1/2	95, 94, 92, 89, 86, 82, 77, 71, 66% sp^{2 2}s; 2,4, 6, 8,11,15, 20, 25, 30% sp^2 2P; 2, 2, 2, 2, 2, 2,1,1,1% sd^{2 2}S
	1/2	93, 92, 90, 88, 85, 81, 76, 71, 67% sp^{2 2}P; 2, 4, 6, 8,12,16, 20, 25, 30% sp^2 2S; 4, 3, 3, 3, 3, 3, 3,3, 3% p²d
	3/2	95, 95, 95, 95, 95, 95, 95, 95, 95% sp^{2 2}P; 5, 4, 4,4,4, 3, 3, 3, 3% p²d
3s²3d	3/2	83, 84, 84, 84, 85, 85, 85, 85, 85% s²d²D; 13, 13, 12, 12, 12, 12, 12, 12, 12% sp^{2 2}D
	5/2	83, 84, 84, 85, 85, 85, 85, 86, 86% s²d²D; 13, 13, 12, 12, 12, 12, 12, 11, 11% sp^{2 2}D

Abstract

Cited By

Figures (5)

Tables (5)

Journal of the Optical Society of America B