Analysis of the Spectrum of Neutral Erbium (Er i)

Nissan Spector

doi:10.1364/JOSA.56.000341

Journal of the Optical Society of America
Vol. 56,
Issue 3,
pp. 341-349
(1966)
•https://doi.org/10.1364/JOSA.56.000341

Analysis of the Spectrum of Neutral Erbium (Er i)

Nissan Spector

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Nissan Spector, "Analysis of the Spectrum of Neutral Erbium (Er i)," J. Opt. Soc. Am. 56, 341-349 (1966)

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Abstract

First results of a continuing analysis of Er i are given: 30 low levels belonging to 4f¹¹5d6s² and other odd configurations, as well as 138 high levels of even parity are assigned J-values. More than 300 absorption lines are classified. The connection of the odd levels to the 4f¹²6s² configuration is established, using transitions in the infrared. The energy matrices in intermediate coupling for the subconfiguration f¹¹(⁴I)d have been calculated and are given. The theoretical formulas were adjusted by a least-squares fit to 19 observed levels designated as $4 f^{11} ({{}^{4}I}_{7 \frac{1}{2}, 6 \frac{1}{2}}) 5 d 6 s^{2}$ resulting in new values for 6 electrostatic and 2 spin-orbit interaction parameters. The rms error was 186 cm⁻¹. Calculated percentage compositions in various coupling schemes show the J₁ − j type to be the best for these levels.

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Odd parity		J	Level (in cm⁻¹)
Configuration	Designation	J	Level (in cm⁻¹)
4f¹¹5d6s²	$({{}^{4}I}_{15 / 2}) d_{1 \frac{1}{2}}$	6	7176.52
		7	7696.97
		9	8620.58
		8	9350.12
	$({{}^{4}I}_{15 / 2}) d_{2 \frac{1}{2}}$	10	9655.86
		9	10557.92
		5	11401.20
		8	11557.68
		6	11799.78
		7	11887.51
	$({{}^{4}I}_{13 / 2}) d_{1 \frac{1}{2}}$	8	15083.12
		5	15185.36
		7	15846.55
		6	16070.10
	$({{}^{4}I}_{13 / 2}) d_{2 \frac{1}{2}}$	9	16501.42
		8	17297.67
		5	17347.86
		6	17456.39
		7	17796.15
	$({{}^{4}I}_{11 / 2}) d_{1 \frac{1}{2}} ?$	7	21168.43
4f¹¹5d²6s ?		6	16321.18
		5	17029.06
		6	17073.80
		7	17157.31
		8	18335.50
		7	18774.12
		5	19201.37
		6	19326.60
		6	20166.13
4f¹²6s6p ?	(³H₆)¹P₁	7	24943.28

Even parity
J	Level (in cm⁻¹)	J	Level (in cm⁻¹)	J	Level (in cm⁻¹)
9	25220.21	7	27459.44	8	28579.02
9	26099.61	8	27578.76	8	28699.86
8	26268.09	7	27625.55	8	29451.90
8	27178.91	9	28043.28	6	29801.24
9	27198.09	8	28397.15	7	29967.87
6	30468.40	7	35667.09	8	38668.32
7	30693.29	7	35717.11	8	38734.25
8	30726.74	7	35833.80	6	38786.55
7	31105.67	6	35963.38	5	38831.97
6	31338.47	6	36026.88	6	38923.59
6	31523.77	7	36051.46	8	39049.48
8	31559.84	7	36123.04	6	39075.90
6	31878.79	9	36136.20	7	39145.46
9	31906.70	6	36306.27	6	39164.27
6	31946.42	9	36321.93	7	39256.46
7	32001.45	8	36384.56	6	39350.52
6	32212.46	7	36418.41	8	39432.67
6	32799.50	10	36461.86	6	39658.19
8	32884.88	9	36494.17	7	39738.48
6	33139.81	6	36511.23	8	39843.43
5	33519.75	5	36710.83	6	39971.07
10	33619.34	10	36712.59	7	40131.34
6	33750.65	7	36735.75	6	40140.64
6	34055.28	6	36876.46	5	40343.43
7	34153.77	7	36891.99	7	40833.99
9	34224.06	8	37021.28	6	40840.94
8	34288.44	6	37044.42	8	41168.16
6	34313.11	9	37062.83	6	41407.83
5	34447.77	7	37178.45	5	41603.85
6	34458.01	8	37378.46	6	41907.33
9	34587.81	7	37391.24	7	41989.93
7	34596.40	6	37542.80	6	42353.85
9	34724.91	8	37645.76	8	42376.27
7	34733.25	7	37806.99	6	42627.57
8	34756.59	8	37843.86	6	43191.63
8	34990.25	8	38164.92	6	43298.22
7	35014.76	9	38172.82	8	43586.06
7	35191.47	8	38253.69	7	43826.67
6	35218.61	7	38301.63	6	43870.49
8	35300.42	8	38343.70	6	44194.78
5	35328.68	9	38487.26	8	44201.05
6	35370.38	7	38545.34	8	44301.52
7	35394.60	8	38556.76	8	44410.89
8	35493.31	6	38604.59	6	44827.91
6	35557.18	7	38664.26	7	45874.42
8	35632.61	6	38667.81	7	46970.82

Parameter	Results from least-squares (in cm⁻¹)
F₀	16666 ±139
F₂	130 ±14
F₄	16 ±4
G₁	98 ±21
G₃	14 ±9
G₅	4.8±0.9
ζ_f	2577 ±39
ζ_d	805 ±44
rms error	186
in percent of total width	1.7%

Designation	J	Percentage composition		Observed (cm⁻¹)	Calculated (cm⁻¹)	O-C (cm⁻¹)	g_obs	g_calc
Designation	J	in J₁ − j coupling	in J₁ − l coupling	Observed (cm⁻¹)	Calculated (cm⁻¹)	O-C (cm⁻¹)	g_obs	g_calc
$({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	6	$93 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$92 % ({{}^{4}I}_{7 \frac{1}{2}}) [5 \frac{1}{2}]$	7177	7349	−172	1.340	1.312
$({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	7	$78 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}} + 18 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$90 % ({{}^{4}I}_{7 \frac{1}{2}}) [6 \frac{1}{2}]$	7697	7916	−219	1.254	1.265
$({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	9	$58 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}} + 31 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$28 % ({{}^{4}I}_{7 \frac{1}{2}}) [9 \frac{1}{2}] + 41 % ({{}^{4}I}_{7 \frac{1}{2}}) [8 \frac{1}{2}] + 31 % ({{}^{4}I}_{6 \frac{1}{2}}) [8 \frac{1}{2}]$	8621	8651	−30		1.163
$({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	8	$75 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}} + 20 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$63 % ({{}^{4}I}_{7 \frac{1}{2}}) [8 \frac{1}{2}] + 36 % ({{}^{4}I}_{7 \frac{1}{2}}) [7 \frac{1}{2}]$	9350	9097	253		1.185
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	10	$100 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$100 % ({{}^{4}I}_{7 \frac{1}{2}}) [9 \frac{1}{2}]$	9656	9269	387		1.200
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	9	$88 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$55 % ({{}^{4}I}_{7 \frac{1}{2}}) [8 \frac{1}{2}] + 38 % ({{}^{4}I}_{7 \frac{1}{2}}) [9 \frac{1}{2}]$	10 558	10 610	−52		1.174
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	5	$81 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$78 % ({{}^{4}I}_{7 \frac{1}{2}}) [5 \frac{1}{2}] + 21 % ({{}^{4}I}_{6 \frac{1}{2}}) [4 \frac{1}{2}]$	11 401	11 491	−90		1.216
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	8	$94 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$64 % ({{}^{4}I}_{7 \frac{1}{2}}) [7 \frac{1}{2}] + 33 % ({{}^{4}I}_{7 \frac{1}{2}}) [8 \frac{1}{2}]$	11 558	11 607	−49		1.182
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	6	$79 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$75 % ({{}^{4}I}_{7 \frac{1}{2}}) [6 \frac{1}{2}]$	11 800	11 811	−11		1.191
$({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	7	$75 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}} + 18 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$83 % ({{}^{4}I}_{7 \frac{1}{2}}) [7 \frac{1}{2}]$	11 888	11 959	−71		1.151
$({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	8	$95 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$81 % ({{}^{4}I}_{6 \frac{1}{2}}) [8 \frac{1}{2}]$	15 083	15 058	25		1.056
$({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	5	$81 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}} + 18 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$61 % ({{}^{4}I}_{6 \frac{1}{2}}) [4 \frac{1}{2}] + 21 % ({{}^{4}I}_{7 \frac{1}{2}}) [5 \frac{1}{2}]$	15 185	15 213	−27		1.189
$({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	7	$90 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$65 % ({{}^{4}I}_{6 \frac{1}{2}}) [7 \frac{1}{2}] + 24 % ({{}^{4}I}_{6 \frac{1}{2}}) [6 \frac{1}{2}]$	15 847	15 744	102		1.073
$({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	6	$79 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$62 % ({{}^{4}I}_{6 \frac{1}{2}}) [5 \frac{1}{2}] + 21 % ({{}^{4}I}_{6 \frac{1}{2}}) [6 \frac{1}{2}]$	16 070	15 946	124		1.152
$({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	9	$62 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}} + 37 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$62 % ({{}^{4}I}_{6 \frac{1}{2}}) [8 \frac{1}{2}] + 34 % ({{}^{4}I}_{7 \frac{1}{2}}) [9 \frac{1}{2}]$	16 501	16 493	8		1.129
	4	$83 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$81 % ({{}^{4}I}_{6 \frac{1}{2}}) [4 \frac{1}{2}] + 18 % ({{}^{4}I}_{5 \frac{1}{2}}) [3 \frac{1}{2}]$		16 948			1.081
$({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	8	$76 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}} + 22 % ({{}^{4}I}_{7 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$83 % ({{}^{4}I}_{6 \frac{1}{2}}) [7 \frac{1}{2}]$	17 298	17 222	76		1.129
$({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	5	$84 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$66 % ({{}^{4}I}_{6 \frac{1}{2}}) [5 \frac{1}{2}]$	17 348	17 349	−1		1.101
$({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	6	$80 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$68 % ({{}^{4}I}_{6 \frac{1}{2}}) [6 \frac{1}{2}] + 19 % ({{}^{4}I}_{6 \frac{1}{2}}) [5 \frac{1}{2}]$	17 456	17 623	−167		1.057
$({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	7	$93 % ({{}^{4}I}_{6 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$68 % ({{}^{4}I}_{6 \frac{1}{2}}) [6 \frac{1}{2}] + 26 % ({{}^{4}I}_{6 \frac{1}{2}}) [7 \frac{1}{2}]$	17 796	17 882	−86		1.121
	7	$90 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$91 % ({{}^{4}I}_{5 \frac{1}{2}}) [7 \frac{1}{2}]$		20 261			0.931
	6	$80 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$84 % ({{}^{4}I}_{5 \frac{1}{2}}) [6 \frac{1}{2}]$		21 196			0.923
	4	$72 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$67 % ({{}^{4}I}_{5 \frac{1}{2}}) [4 \frac{1}{2}] + 18 % ({{}^{4}I}_{5 \frac{1}{2}}) [3 \frac{1}{2}]$		21 329			0.956
	3	$88 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$87 % ({{}^{4}I}_{5 \frac{1}{2}}) [3 \frac{1}{2}]$		21 748			0.828
	5	$83 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{1 \frac{1}{2}}$	$78 % ({{}^{4}I}_{5 \frac{1}{2}}) [5 \frac{1}{2}]$		21 990			0.916
	4	$75 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$63 % ({{}^{4}I}_{5 \frac{1}{2}}) [3 \frac{1}{2}] + 22 % ({{}^{4}I}_{5 \frac{1}{2}}) [4 \frac{1}{2}]$		22 513			1.003
	8	$97 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$97 % ({{}^{4}I}_{5 \frac{1}{2}}) [7 \frac{1}{2}]$		22 795			1.032
	5	$78 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$70 % ({{}^{4}I}_{5 \frac{1}{2}}) [4 \frac{1}{2}]$		23 095			0.991
	7	$94 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$93 % ({{}^{4}I}_{5 \frac{1}{2}}) [6 \frac{1}{2}]$		23 265			1.035
	6	$81 % ({{}^{4}I}_{5 \frac{1}{2}}) d_{2 \frac{1}{2}}$	$83 % ({{}^{4}I}_{5 \frac{1}{2}}) [5 \frac{1}{2}]$		23 687			1.009

Odd parity		J	Level (in cm⁻¹)
Configuration	Designation	J	Level (in cm⁻¹)
4f¹¹5d6s²	$({{}^{4}I}_{15 / 2}) d_{1 \frac{1}{2}}$	6	7176.52
		7	7696.97
		9	8620.58
		8	9350.12
	$({{}^{4}I}_{15 / 2}) d_{2 \frac{1}{2}}$	10	9655.86
		9	10557.92
		5	11401.20
		8	11557.68
		6	11799.78
		7	11887.51
	$({{}^{4}I}_{13 / 2}) d_{1 \frac{1}{2}}$	8	15083.12
		5	15185.36
		7	15846.55
		6	16070.10
	$({{}^{4}I}_{13 / 2}) d_{2 \frac{1}{2}}$	9	16501.42
		8	17297.67
		5	17347.86
		6	17456.39
		7	17796.15
	$({{}^{4}I}_{11 / 2}) d_{1 \frac{1}{2}} ?$	7	21168.43
4f¹¹5d²6s ?		6	16321.18
		5	17029.06
		6	17073.80
		7	17157.31
		8	18335.50
		7	18774.12
		5	19201.37
		6	19326.60
		6	20166.13
4f¹²6s6p ?	(³H₆)¹P₁	7	24943.28

Wavelength (in Å)	Intensity	Even level		Odd level
Wavelength (in Å)	Intensity	(cm⁻¹)	J	(cm⁻¹)	J
9927.10^a	30	6958	5	17029	5
9883.18^a	3	6958	5	17073	6
9849.38^a	80	5035	4	15185	5
9622.45^a	8	6958	5	17347	5
9523.00^a	80	6958	5	17456	6
8119.47^a	80	5035	4	17437	5
6583.48^a	60	0	6	15185	5
5870.69^a	1	0	6	17029	5
5726.98^a	3	0	6	17456	6
5909.28	1	26268	8	9350	8
5855.33	5	0	6	17073	6
5826.78	12	0	6	17157	7
5762.77	5	0	6	17347	5
5719.49	1	26099	9	8620	9
5348.02	2	28043	9	9350	8
5172.74	2	0	6	19326	6
4722.71	50	0	6	21168	7
4713.09	2	38667	6	17456	6
4710.87	1 F	31542	6	16321	6
4687.80	3	36511	6	15185	5
4684.73	1 F	33139	6	11799	6
4684.01	1 F	30693	7	9350	8
4640.20	1	37391	7	15846	7
4522.71	2	29801	6	7696	7
4488.85	2	29967	7	7696	7
4432.03	1	31906	9	9350	8
4418.68	3	29801	6	7176	6
4390.21	1	30468	6	7696	7
4386.37	10	29967	7	7176	6
4380.63	2	38667	6	15846	7
4359.16	1	34733	7	11799	6
4347.27	1	30693	7	7696	7
4340.92	20	34587	9	11557	8
4313.66	1	34733	7	11557	8
4306.33	1	35014	7	11799	6
4301.21	1	44410	8	21168	7
4293.16	1	31906	9	8620	9
4270.68	1	31105	7	7696	7
4269.88	1	35300	8	11887	7
4251.06	2	30693	7	7176	6
4221.07	1	40840	6	17157	7
4212.74	1	34288	8	10557	9
4197.39	1	35218	6	11401	5
4195.73	1	31523	6	7696	7
4177.79	1	31105	7	7176	6
4171.81	3	33619	10	9655	10
4170.82	1	35370	6	11401	5
4160.29	2	34587	9	10557	9
4113.27	2	32001	7	7696	7
4091.75	1	34990	8	10557	9
4070.52	1	41907	6	17347	7
4069.08	1	34224	9	9655	10
4067.41	1 VF	36136	9	11557	8
4027.04	2	32001	7	7176	6
4009.75	3	34587	9	9655	10
4007.97	600 VW	0	6	24943	7
3999.04	1	33619	10	8620	9
3993.08	1 F	32212	6	7176	6
3982.50	1	32799	6	7696	7
3981.32	1	36511	6	11401	5
3977.57	1	37021	8	11887	7
3969.01	1	32884	8	7696	7
3961.20	8	34587	9	9350	8
3959.86	1 VF	34596	7	9350	8
3948.05	3	41168	8	15846	7
3939.79	1	34724	9	9350	8
3938.49	1	34733	7	9350	8
3936.58	8	43191	6	17796	7
3934.89	1	34756	8	9350	8
3929.28	8	33139	6	7696	7
3919.65	1 VF	37062	9	11557	8
3908.44	2	36136	9	10557	9
3904.60	2	34224	9	8620	9
3901.64	3	32799	6	7176	6
3899.04	10	34990	8	9350	8
3896.75	1	37542	6	11887	7
3895.34	2	35014	7	9350	8
3894.85	1	34288	8	8620	9
3881.17	1 W	37645	8	11887	7
3880.30	1	36321	9	10557	9
3871.75	2	37378	8	11557	8
3870.86	2 VW	36384	8	10557	9
3869.84	2	37391	7	11557	8
3868.67	1	35191	7	9350	8
3859.31	3	36461	10	10557	9
3854.51	2	36494	9	10557	9
3852.42	2	43298	6	17347	5
3849.92	40	34587	9	8620	9
3838.50	10	35394	7	9350	8
3837.17	3	33750	6	7696	7
3832.53	2	41168	8	15083	8
3829.70	1	34724	9	8620	9
3825.05	1	34756	8	8620	9
3824.24	1	37542	6	11401	5
3823.98	2	41989	7	15846	7
3822.33	1	36712	10	10557	9
3803.73	8	35632	8	9350	8
3803.19	2	37843	8	11557	8
3794.91	1	33519	5	7176	6
3792.79	80	34055	6	7696	7
3791.55	20	35717	7	9350	8
3791.16	25	34990	8	8620	9
3784.78	1	43870	6	17456	6
3778.68	50	34153	7	7696	7
3777.76	2	37021	8	10557	9
3775.33	15	36136	9	9655	10
3774.84	8	35833	7	9350	8
3771.81	10	37062	9	10557	9
3761.99	50	33750	6	7176	6
3759.54	30	34288	8	7696	7
3756.18	1	38172	9	11557	8
3756.06	50	34313	6	7696	7
3749.03	8	36321	9	9655	10
3747.09	2	35300	8	8620	9
3738.10	1 F	38301	7	11557	8
3735.72	20	34458	6	7696	7
3732.96	2	38668	8	11887	7
3732.23	8	36136	9	9350	8
3729.46	5	36461	10	9655	10
3727.43	1	37378	8	10557	9
3724.96	10	36494	9	9655	10
3723.80	1 F	38734	8	11887	7
3721.35	1	38664	7	11799	6
3720.83	1	38667	6	11799	6
3720.21	2	35493	8	8620	9
3719.37	20	34055	6	7176	6
3716.51	8	34596	7	7696	7
3712.35	1 VF	38487	9	11557	8
3706.52	20	36321	9	9350	8
3705.77	10	34153	7	7176	6
3704.46	1	38786	6	11799	6
3702.77	1	38556	8	11557	8
3700.99	3	35632	8	8620	9
3698.20	1 F	38831	5	11799	6
3697.93	1	36384	8	9350	8
3697.72	250	34733	7	7696	7
3694.90	15	36712	10	9655	10
3694.49	15	34756	8	7696	7
3693.33	3	36418	7	9350	8
3690.67	8	37645	8	10557	9
3688.09	1	38664	7	11557	8
3687.53	40	38668	8	11557	8
3684.01	1	34313	6	7176	6
3683.00	20	36494	9	9350	8
3678.58	3	38734	8	11557	8
3667.60	1	39145	7	11887	7
3666.44	1	38667	6	11401	5
3665.81	2	34447	5	7176	6
3665.12	15 VW	39075	6	11799	6
3664.44	60	34458	6	7176	6
3663.84	8	37843	8	10557	9
3662.85	25	34990	8	7696	7
3659.56	20	35014	7	7696	7
3655.82	8 W	39145	7	11799	6
3653.20	1	39164	6	11799	6
3650.52	1 F	36735	7	9350	8
3647.64	3	37062	9	9655	10
3644.48	1	38831	5	11401	5
3641.72	1 W	43298	6	15846	7
3641.05	1	39256	7	11799	6
3640.21	3	39350	6	11887	7
3636.39	15	39049	8	11557	8
3636.04	3	35191	7	7696	7
3633.25	20	36136	9	8620	9
3632.45	3	35218	6	7696	7
3629.79	1 VF	36891	7	9350	8
3629.37	25	39432	8	11887	7
3628.62	10	39350	6	11799	6
3627.82	30	34733	7	7176	6
3623.74	2	39145	7	11557	8
3621.23	1	38164	8	10557	9
3620.17	200	38172	9	10557	9
3612.83	20	37021	8	9350	8
3612.54	10	35370	6	7696	7
3612.36	1	39075	6	11401	5
3609.63	2	38253	8	10557	9
3609.37	10	35394	7	7696	7
3608.88	30	36321	9	8620	9
3607.42	20	37062	9	9350	8
3603.93	1 F	43586	8	15846	7
3601.75	1	43826	7	16070	6
3600.86	2	39164	6	11401	5
3600.75	2	36384	8	8620	9
3599.88	5	39658	6	11887	7
3597.94	1 VF	38343	8	10557	9
3596.55	2	35493	8	7696	7
3596.09	4	44301	8	16501	9
3592.44	1	37178	7	9350	8
3591.14	5	35014	7	7176	6
3590.75	50	36461	10	8620	9
3589.52	3	39738	7	11887	7
3588.57	3	39658	6	11799	6
3588.35	30	35557	6	7696	7
3586.59	15	44194	6	16321	6
3586.40	3	39432	8	11557	8
3579.44	20	38487	9	10557	9
3578.23	8	39738	7	11799	6
3576.85	2	39350	6	11401	5
3576.02	1	39843	8	11887	7
3574.22	3	35667	7	7696	7
3570.55	8	38556	8	10557	9
3569.58	1 VF	43191	6	15185	5
3568.49	8	35191	7	7176	6
3567.82	8	35717	7	7696	7
3567.33	1 VF	43870	6	15846	7
3566.79	1	37378	8	9350	8
3565.16	10	37391	7	9350	8
3565.05	1	35218	6	7176	6
3559.80	1 VF	39971	6	11887	7
3558.72	50	36712	10	8620	9
3556.38	20	38668	8	10557	9
3556.07	8	43298	6	15185	5
3553.05	20	35833	7	7696	7
3551.10	5	35328	5	7176	6
3548.07	8	38734	8	10557	9
3547.51	3	39738	7	11557	8
3545.88	80	35370	6	7176	6
3542.81	15	35394	7	7176	6
3539.59	80	40131	7	11887	7
3538.38	1 W	40140	6	11887	7
3536.76	8	35963	6	7696	7
3534.35	5	39843	8	11557	8
3528.85	1	36026	6	7696	7
3526.55	1	44194	6	15846	7
3525.78	2	44201	8	15846	7
3522.52	80	35557	6	7176	6
3520.05	80	37021	8	8620	9
3516.91	10	36123	7	7696	7
3514.90	10	37062	9	8620	9
3513.05	100 VW	37806	7	9350	8
3508.95	20	35667	7	7176	6
3508.82	20	39049	8	10557	9
3508.57	20	37843	8	9350	8
3507.43	1	43586	8	15083	8
3505.70	30	38172	9	9655	10
3502.78	300 VW	35717	7	7176	6
3502.39	2 VV	40343	5	11799	6
3498.74	3	40131	7	11557	8
3495.81	1	38253	8	9655	10
3494.39	5	36306	6	7696	7
3488.53	30	35833	7	7176	6
3484.83	1 F	36384	8	7696	7
3480.74	40	36418	7	7696	7
3478.56	4	40140	6	11401	5
3478.07	1	43826	7	15083	8
3476.32	20	37378	8	8620	9
3472.83	5	35963	6	7176	6
3469.48	200 VW	36511	6	7696	7
3468.46	1	38172	9	9350	8
3465.16	100	36026	6	7176	6
3462.24	30	39432	8	10557	9
3458.80	20	38253	8	9350	8
3454.15	1 VF	40343	5	11401	5
3453.65	20	40833	7	11887	7
3453.08	1	38301	7	9350	8
3452.83	1	40840	6	11887	7
3448.05	8	38343	8	9350	8
3444.29	20	37645	8	8620	9
3443.20	2	40833	7	11799	6
3442.71	50	36735	7	7696	7
3442.42	2	40840	6	11799	6
3431.91	2	36306	6	7176	6
3431.07	2	38487	9	9350	8
3426.08	2	36876	6	7696	7
3424.26	15	36891	7	7696	7
3422.91	20	38556	8	9350	8
3421.55	1 F	44301	8	15083	8
3420.95	30	37843	8	8620	9
3418.78	5	36418	7	7176	6
3414.76	3	40833	7	11557	8
3414.25	1	41168	8	11887	7
3413.68	1	39843	8	10557	9
3410.35	3	38664	7	9350	8
3409.87	15	38668	8	9350	8
3409.16	3	37021	8	7696	7
3407.95	2	36511	6	7176	6
3406.47	2	37044	6	7696	7
3395.81	5	40840	6	11401	5
3390.99	10	37178	7	7696	7
3386.53	1 VF	41407	6	11887	7
3384.92	1	36710	5	7176	6
3383.77	15	38164	8	8620	9
3382.86	10	38172	9	8620	9
3382.08	30	36735	7	7176	6
3373.63	5	38253	8	8620	9
3369.10	1 F	46970	7	17297	8
3368.18	200	37378	8	7696	7
3366.70	20	37391	7	7696	7
3366.11	2	39049	8	9350	8
3364.29	20	36891	7	7176	6
3363.42	2	38343	8	8620	9
3354.25	2	45874	7	16070	6
3349.60	8	37542	6	7696	7
3347.27	5	38478	9	8620	9
3342.79	1	39256	7	9350	8
3339.49	20	38556	8	8620	9
3338.09	3	37645	8	7696	7
3332.18	10	37178	7	7176	6
3327.08	20	38668	8	8620	9
3323.23	20	39432	8	9350	8
3319.80	2	38734	8	8620	9
3316.15	5	37843	8	7696	7
3308.70	8	37391	7	7176	6
3292.19	1	37542	6	7176	6
3285.42	1	39049	8	8620	9
3281.20	8	38164	8	7696	7
3278.47	2	39843	8	9350	8
3271.63	2	38253	8	7696	7
3266.53	3	38301	7	7696	7
3263.79	5	37806	7	7176	6
3262.04	3	38343	8	7696	7
3246.74	3	45874	7	15083	8
3244.55	2	39432	8	8620	9
3239.51	6	38556	8	7696	7
3228.30	3	38664	7	7696	7
3227.85	8	38668	8	7696	7
3215.61	1	38786	6	7696	7
3211.94	1	38301	7	7176	6
3201.87	10	39843	8	8620	9
3201.47	2	38923	6	7696	7
3193.58	1 VF	43191	6	11887	7
3188.59	2	39049	8	7696	7
3186.94	1	38545	7	7176	6
3185.93	2	39075	6	7696	7
3182.70	1 VF	43298	6	11887	7
3175.32	1	40833	7	9350	8
3174.95	2	38664	7	7176	6
3174.57	3	38667	6	7176	6
3173.84	1 F	43298	6	11799	6
3162.67	1	38786	6	7176	6
3153.83	1	43586	8	11887	7
3150.12	10	39432	8	7696	7
3141.96	1	41168	8	9350	8
3133.94	2	39075	6	7176	6
3130.04	2	43826	7	11887	7
3127.88	2	39658	6	7696	7
3127.13	2	39145	7	7176	6
3121.48	2	43826	7	11799	6
3120.04	1	39738	7	7696	7
3117.20	5	43870	6	11799	6
3098.06	1	43826	7	11557	8
3094.38	3	44194	6	11887	7
3086.01	2	44194	6	11799	6
3082.24	20	40131	7	7696	7
3078.94	20	43870	6	11401	5
3077.74	2	39658	6	7176	6
3073.80	1	44410	8	11887	7
3062.51	1	44201	8	11557	8
3053.13	10	44301	8	11557	8
3042.97	20	44410	8	11557	8
3033.57	2	40131	7	7176	6
3027.01	2	42376	8	9350	8
3016.90	1	40833	7	7696	7
3016.26	2	40840	6	7696	7
3014.17	3	40343	5	7176	6
2990.78	1	44827	6	11401	5
2971.51	2	44201	8	10557	9
2969.63	1	40840	6	7176	6
2965.55	4	41407	6	7696	7
2962.66	10	44301	8	10557	9
2920.05	10	43586	8	9350	8
2882.72	10	42376	8	7696	7
2871.62	1	41989	7	7176	6
2859.12	1	43586	8	8620	9
2851.36	1	44410	8	9350	8
2785.53	1 UR	43586	8	7696	7
2816.48	2	43191	6	7696	7
2809.71	1	44201	8	8620	9
2801.74	20	44301	8	8620	9
2793.22	1	44410	8	8620	9
2785.53	1 UR	43586	8	7696	7
2767.01	1 F	43826	7	7696	7
2738.60	2	44201	8	7696	7
2731.10	3	44301	8	7696	7
2724.45	1	43870	6	7176	6

Abstract

Cited By

Figures (3)

Tables (5)

Equations (3)

Journal of the Optical Society of America