VizieR

CfA VizieR . ADAC VizieR . Cambridge (UK) VizieR . IUCAA VizieR . INASAN VizieR .

VizieR

J/ApJS/215/20/table1 Vanadium log(gf) and transition probabilities (Lawler+, 2014)
Fourier Transform Spectra of a custom water-cooled V Hollow Cathode Discharge (HCD) lamp (14 rows)
 
Full

Seq

Date
"Y:M:D"
Num

Gas

iLamp
mA
Wave1
cm-1
Wave2
cm-1
Lim
cm-1
coadd

Beam

Filt

Det

1 11984-12-09 3Ar-Ne 600 776449105 0.05712UV  Mid Range Si Diode
2 21984-12-09 4Ar-Ne 300 776449105 0.057 8UV  Mid Range Si Diode
3 31984-12-09 5Ar-Ne 150 776449105 0.057 8UV  Mid Range Si Diode
4 41986-07-30 9Ar 5001492437018 0.048 4UVCuSO4Large UV Si Diode
5 51986-07-3010Ar 5001492437018 0.048 4UVCuSO4Large UV Si Diode
6 61981-06-16 7Ar 332 692437564 0.043 8UVWG295UV Mid Range Si Diode
7 71981-06-15 3Ar 2501487836533 0.043 8UVCuSO4 WG295UV Mid Range Si Diode
8 81979-12-12 9Ar 3001242231054 0.04210UVTC+ 4-97 WG345Mid Range Si Diode
9 91979-12-12 8Ar 300 771622421 0.030 8UVGG945Super Blue Si Diode
10101980-09-04 1Ar 110 017837 0.023 5UVRG610InSb
11111983-11-30 3Ar 460 2799 9518 0.01117CaF2SiInSb
12121983-04-17 4Ne-Ar 370 1534 5769 0.01180CaF2GeInSb
13131984-07-25 5Ne10001294845407 0.054 8UVCuSO4R166 photomultiplier Mid Range Si Diode
14141983-11-30 4Ne 510 2799 9517 0.01116CaF2SiInSb
J/ApJS/215/20/table2 Vanadium log(gf) and transition probabilities (Lawler+, 2014)
Echelle spectra of commercial V HCD lamps and a custom water-cooled V HCD lamp (19 rows)
 
Full

imin

imax

Date
"Y:M:D"
Num

Gas

iLamp
mA
Wave1
0.1nm
Wave2
0.1nm
Res

coadd

Exp
s
1 47 512013-05-241, 3, 5, 7, 9Ne 322003900250000 60 90
2 52 562013-05-211, 3, 5, 7, 9Ne 522003900250000 90 60
3 57 612013-05-221, 3, 5, 7, 9Ne1022003900250000 90 60
4 62 662013-05-231, 3, 5, 7, 9Ne1522003900250000 60 90
5 67 712013-05-201, 3, 5, 7, 9Ar 322003900250000 6900
6 72 762013-05-151, 3, 5, 7, 9Ar 522003900250000 18300
7 77 812013-05-161, 3, 5, 7, 9Ar1022003900250000 88 60
8 82 862013-05-171, 3, 5, 7, 9Ar1222003900250000 60 90
9 87 912014-01-301, 3, 5, 7, 9Ne 520002800250000 18300
10 92 962014-01-311, 3, 5, 7, 9Ne1020002800250000 36150
11 971012014-02-031, 3, 5, 7, 9Ne1520002800250000 72 75
121021062014-02-051, 3, 5, 7, 9Ar1520002800250000 45120
131071112014-04-241, 3, 5, 7, 9Ar3221003200250000 30120
141121162014-04-161, 3, 5, 7, 9Ar4021003200250000 20180
151171212014-04-171, 3, 5, 7, 9Ar4021003200250000 20180
161221262014-04-281, 3, 5, 7, 9Ar5021003200250000 20180
171271312014-05-131, 3, 5, 7, 9Ar1021003200250000 40180
181321362014-05-091, 3, 5, 7, 9Ar1521003200250000 90 60
191371412014-05-141, 3, 5, 7, 9Ne1521003200250000120 45
J/ApJS/215/20/table3 Vanadium log(gf) and transition probabilities (Lawler+, 2014)
Experimental Atomic Transition Probabilities for 836 lines of VI organized by increasing wavelength in air (836 rows)
 
Full

lamAir
0.1nm
E1
cm-1
P1

J1

E0
cm-1
P0

J0

A
10+6/s
e_
(...)
log(gf)

12384.287041928.473o 0.5 0.000e 1.5 4.9000 0.5000-2.08
22401.903741758.357o 3.5 137.383e 2.5 8.6000 1.6000-1.22
32406.747541860.647o 4.5 323.432e 3.5 9.4000 1.6000-1.09
42412.689541758.357o 3.5 323.432e 3.5 10.8000 2.1000-1.12
52420.121441860.647o 4.5 552.955e 4.5 10.0000 1.7000-1.06
62426.129741758.357o 3.5 552.955e 4.5 1.0800 0.2100-2.12
72501.613939962.150o 2.5 0.000e 1.5 12.2000 2.0000-1.16
82503.303739935.176o 1.5 0.000e 1.5 11.4000 2.6000-1.37
92506.906639877.786o 0.5 0.000e 1.5 51.0000 7.0000-1.01
102507.862739999.966o 2.5 137.383e 2.5 12.3000 2.3000-1.16
112511.945839935.176o 1.5 137.383e 2.5 31.0000 4.0000-0.94
122517.148640038.970o 4.5 323.432e 3.5 14.2000 2.1000-0.87
132519.623339999.966o 2.5 323.432e 3.5 40.0000 5.0000-0.64
142530.185340063.874o 5.5 552.955e 4.5 14.4000 2.1000-0.78
152545.924139266.680o 1.5 0.000e 1.5 17.7000 2.7000-1.16
162549.968839341.784o 3.5 137.383e 2.5 1.8000 0.5000-1.85
172554.863439266.680o 1.5 137.383e 2.5 3.6000 0.9000-1.85
182562.128439341.784o 3.5 323.432e 3.5 16.7000 2.4000-0.88
192574.018739391.079o 4.5 552.955e 4.5 17.1000 3.0000-0.77
202577.290139341.784o 3.5 552.955e 4.5 2.8000 0.6000-1.66
212642.263737835.065o 1.5 0.000e 1.5 8.1000 0.7000-1.47
222643.154737959.695o 2.5 137.383e 2.5 6.4000 0.8000-1.40
232645.257138115.684o 3.5 323.432e 3.5 11.3000 1.2000-1.02
242647.705437757.309o 0.5 0.000e 1.5 49.0000 4.0000-0.98
252651.893537835.065o 1.5 137.383e 2.5 33.2000 2.1000-0.85
262656.221437959.695o 2.5 323.432e 3.5 34.0000 3.0000-0.67
272661.421638115.684o 3.5 552.955e 4.5 32.0000 3.0000-0.57
282671.669937556.034o 3.5 137.383e 2.5 4.2000 0.7000-1.45
292678.656837644.487o 4.5 323.432e 3.5 4.0000 0.7000-1.37
302685.020837556.034o 3.5 323.432e 3.5 0.5400 0.2100-2.33
312686.509737764.923o 5.5 552.955e 4.5 3.5000 0.6000-1.34
322722.554247611.858o 4.510892.520e 3.5141.000010.0000 0.20
332731.341547701.807o 5.511100.596e 4.5144.000010.0000 0.29
342838.059135224.990o 2.5 0.000e 1.5 0.4200 0.0900-2.52
352848.773135092.518o 1.5 0.000e 1.5 10.1000 0.5000-1.31
362849.171835224.990o 2.5 137.383e 2.5 7.8000 0.4000-1.24
372851.751035379.307o 3.5 323.432e 3.5 4.1600 0.2400-1.39
382855.222135013.259o 0.5 0.000e 1.5 49.9000 2.5000-0.91
392859.970035092.518o 1.5 137.383e 2.5 35.9000 1.8000-0.75
402864.360635224.990o 2.5 323.432e 3.5 30.4000 1.6000-0.65
412870.546335379.307o 3.5 552.955e 4.5 27.9000 1.5000-0.56
422887.690534619.598o 2.5 0.000e 1.5 0.2600 0.0600-2.72
432888.512634747.128o 3.5 137.383e 2.5 0.1800 0.0400-2.75
442894.571934537.299o 1.5 0.000e 1.5 4.2700 0.2500-1.67
452898.811734486.787o 2.5 0.000e 1.5 0.3800 0.0500-2.55
462899.196134619.598o 2.5 137.383e 2.5 7.2000 0.6000-1.26
472899.598734477.427o 0.5 0.000e 1.5 34.0000 1.9000-1.07
482903.696634428.773o 1.5 0.000e 1.5 6.2000 0.4000-1.50
492904.124834747.128o 3.5 323.432e 3.5 7.0000 0.6000-1.15
502906.132534537.299o 1.5 137.383e 2.5 31.0000 1.7000-0.80
Result truncated to 50 rows
J/ApJS/215/20/table4 Vanadium log(gf) and transition probabilities (Lawler+, 2014)
Hyperfine Structure (HFS) A coefficients for 25 odd parity levels and one even parity level of neutral vanadium from least-square fits to line profiles in Fourier Transfrom Spectrometer (FTS) data (26 rows)
 
Full

Config

Term

2J

E
cm-1
A
mK
13d4(5D)4pz4Po 124770.673-26.6
23d4(5D)4pz4Po 324915.151 -9.7
33d4(5D)4pz4Po 525131.002 -3.1
43d4(5D)4py6Fo 524898.804 3.3
53d4(5D)4py6Fo 724992.909 2.5
63d4(5D)4py6Fo 925111.473 2.1
73d4(5D)4py6Fo1125253.457 2.0
83d4(5D)4py6Do 526505.953 0.5
93d4(5D)4py6Do 726604.807 1.9
103d4(5D)4py6Do 926738.323 3.1
113d3(4P)4s4p(3P)y6Po 329202.790 18.0
123d3(4P)4s4p(3P)y6Po 529296.430 13.0
133d3(4P)4s4p(3P)y6Po 729418.119 15.2
143d3(4F)4s4p(1P)x4Go 531397.822 20.1
153d3(4F)4s4p(1P)x4Go 731541.167 9.7
163d3(4F)4s4p(1P)x4Go 931721.780 5.3
173d3(4F)4s4p(1P)x4Go1131937.131 2.7
183d3(4F)4s4p(1P)w4Fo 532846.822 8.6
193d3(4F)4s4p(1P)w4Fo 732988.845 3.6
203d4(3H)4pz4Io1537518.445 6.1
213d4(a3P)4pt4Do 337835.065 7.1
223d4(a3P)4pt4Do 738115.684 4.8
233d4(3H)4px2Ho 938123.795 10.0
243d4(3H)4px2Ho1138220.663 10.4
253d4(a3F)4pu4Fo 939391.079 9.5
263d34s(5F)5se6F1137931.460 21.1
J/ApJS/215/20/table5 Vanadium log(gf) and transition probabilities (Lawler+, 2014)
*Hyperfine structure line component patterns for 94 transitions of 51VI (1480 rows) (Note)
 
Full

Wave
cm-1
lamAir
0.1nm
F1

F0

dWave
cm-1
dLam
0.1nm
Str

132709.4393056.3328 6 6-0.01853 0.001732 0.22569
232709.4393056.3328 6 5 0.04581-0.004281 0.04514
332709.4393056.3328 5 6-0.07013 0.006554 0.04514
432709.4393056.3328 5 5-0.00579 0.000541 0.11546
532709.4393056.3328 5 4 0.04779-0.004466 0.06857
632709.4393056.3328 4 5-0.04879 0.004559 0.06857
732709.4393056.3328 4 4 0.00479-0.000448 0.04527
832709.4393056.3328 4 3 0.04763-0.004450 0.07366
932709.4393056.3328 3 4-0.02961 0.002767 0.07366
1032709.4393056.3328 3 3 0.01323-0.001236 0.00868
1132709.4393056.3328 3 2 0.04534-0.004236 0.06349
1232709.4393056.3328 2 3-0.01257 0.001175 0.06349
1332709.4393056.3328 2 2 0.01954-0.001825 0.00050
1432709.4393056.3328 2 1 0.04093-0.003825 0.04018
1532709.4393056.3328 1 2 0.00234-0.000218 0.04018
1632709.4393056.3328 1 1 0.02373-0.002218 0.02232
1732665.4133060.4522 7 7-0.05799 0.005433 0.20833
1832665.4133060.4522 7 6 0.00040-0.000037 0.02604
1932665.4133060.4522 6 7-0.08319 0.007794 0.02604
2032665.4133060.4522 6 6-0.02480 0.002324 0.13542
2132665.4133060.4522 6 5 0.02520-0.002361 0.04167
2232665.4133060.4522 5 6-0.04640 0.004348 0.04167
2332665.4133060.4522 5 5 0.00360-0.000337 0.08185
2432665.4133060.4522 5 4 0.04523-0.004238 0.04836
2532665.4133060.4522 4 5-0.01440 0.001350 0.04836
2632665.4133060.4522 4 4 0.02723-0.002551 0.04464
2732665.4133060.4522 4 3 0.06052-0.005670 0.04762
2832665.4133060.4522 3 4 0.01283-0.001202 0.04762
2932665.4133060.4522 3 3 0.04612-0.004321 0.02083
3032665.4133060.4522 3 2 0.07107-0.006659 0.04092
3132665.4133060.4522 2 3 0.03532-0.003309 0.04092
3232665.4133060.4522 2 2 0.06027-0.005647 0.00744
3332665.4133060.4522 2 1 0.07690-0.007205 0.02976
3432665.4133060.4522 1 2 0.05307-0.004972 0.02976
3532665.4133060.4522 1 1 0.06970-0.006531 0.00149
3632665.4133060.4522 1 0 0.07801-0.007309 0.01563
3732665.4133060.4522 0 1 0.06610-0.006193 0.01563
3831403.7843183.4090 7 6 0.02504-0.002538 0.23437
3931403.7843183.4090 6 6-0.04286 0.004345 0.03385
4031403.7843183.4090 6 5 0.02149-0.002178 0.16927
4131403.7843183.4090 5 6-0.10106 0.010245 0.00260
4231403.7843183.4090 5 5-0.03671 0.003722 0.05320
4331403.7843183.4090 5 4 0.01687-0.001710 0.11607
4431403.7843183.4090 4 5-0.08521 0.008638 0.00670
4531403.7843183.4090 4 4-0.03163 0.003207 0.06027
4631403.7843183.4090 4 3 0.01120-0.001136 0.07366
4731403.7843183.4090 3 4-0.07043 0.007140 0.01116
4831403.7843183.4090 3 3-0.02760 0.002798 0.05729
4931403.7843183.4090 3 2 0.00451-0.000457 0.04092
5031403.7843183.4090 2 3-0.05670 0.005748 0.01488
Result truncated to 50 rows
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