Electronic gJ Factors, Natural Lifetimes, and Electric Quadrupole Interaction for Rb 87 in the np ^(2)P_(3/2) Series of the Rb I Spectrum
(1971) In Physica Scripta 4(6). p.269-273- Abstract
- For Rb 87 the level crossing method was applied to the first four levels ( n = 5, 6, 7, and 8) of the np 2 P 3/2 series in the Rb I spectrum. By using magnetic dipole interaction constants from corresponding zero field optical double resonance experiments, the electronic g J factors of 5, 6, and 7 p 2 P 3/2 were calculated from the level crossing data. For these levels the natural radiative lifetimes were determined from the half-widths of the level crossing signals. For 8 p 2 P 3/2 the a factor was obtained assuming g J = -1.336 (2). From the measured electric quadrupole interaction constants b , decreasing values of the nuclear quadrupole moment Q were obtained in 5, 6, 7, and 8 p 2 P 3/2 . When core polarization effects are taken into... (More)
- For Rb 87 the level crossing method was applied to the first four levels ( n = 5, 6, 7, and 8) of the np 2 P 3/2 series in the Rb I spectrum. By using magnetic dipole interaction constants from corresponding zero field optical double resonance experiments, the electronic g J factors of 5, 6, and 7 p 2 P 3/2 were calculated from the level crossing data. For these levels the natural radiative lifetimes were determined from the half-widths of the level crossing signals. For 8 p 2 P 3/2 the a factor was obtained assuming g J = -1.336 (2). From the measured electric quadrupole interaction constants b , decreasing values of the nuclear quadrupole moment Q were obtained in 5, 6, 7, and 8 p 2 P 3/2 . When core polarization effects are taken into account, the different 2 P 3/2 levels yield consistent values for the quadrupole moment. We find ----- -- g J (5 p 2 P 3/2 ) = -1.3362 (6) -- g J (6 p 2 P 3/2 ) = -1.3347 (10) ----- -- Ï (5 p 2 P 3/2 ) = 25.8 (8) ns -- Ï (6 p 2 P 3/2 ) = 111 (3) ns ----- -- b (5 p 2 P 3/2 ) = 12.510 (57) MHz -- b (6 p 2 P 3/2 ) = 3.947 (13) MHz ----- -- Q (5 p 2 P 3/2 ) = 0.131 barn -- Q (6 p 2 P 3/2 ) = 0.133 barn ----- -- g J (7 p 2 P 3/2 ) = -1.3359 (11) -- a (8 p 2 P 3/2 ) = 6.747 (14) MHz ----- -- Ï (7 p 2 P 3/2 ) = 233 (10) ns -- b (8 p 2 P 3/2 ) = 0.933 (20) MHz ----- -- b (7 p 2 P 3/2 ) = 1.768 (8) MHz -- Q (8 p 2 P 3/2 ) = 0.131 barn ----- -- Q (7 p 2 P 3/2 ) = 0.133 barn -- ----- Considering possible sources of error in the evaluation of the quadrupole moment we obtain Q (Rb 87 ) = +0.132 (9) barn. (Less)
Please use this url to cite or link to this publication:
https://lup.lub.lu.se/record/2257459
- author
- Belin, G and Svanberg, Sune LU
- organization
- publishing date
- 1971
- type
- Contribution to journal
- publication status
- published
- subject
- in
- Physica Scripta
- volume
- 4
- issue
- 6
- pages
- 269 - 273
- publisher
- IOP Publishing
- external identifiers
-
- scopus:84921186114
- ISSN
- 0031-8949
- DOI
- 10.1088/0031-8949/4/6/006
- language
- English
- LU publication?
- yes
- id
- 6f8fb0f8-e330-4576-b79b-918ddad57d21 (old id 2257459)
- date added to LUP
- 2016-04-04 14:29:31
- date last changed
- 2021-09-26 03:56:13
@article{6f8fb0f8-e330-4576-b79b-918ddad57d21,
abstract = {{For Rb 87 the level crossing method was applied to the first four levels ( n = 5, 6, 7, and 8) of the np 2 P 3/2 series in the Rb I spectrum. By using magnetic dipole interaction constants from corresponding zero field optical double resonance experiments, the electronic g J factors of 5, 6, and 7 p 2 P 3/2 were calculated from the level crossing data. For these levels the natural radiative lifetimes were determined from the half-widths of the level crossing signals. For 8 p 2 P 3/2 the a factor was obtained assuming g J = -1.336 (2). From the measured electric quadrupole interaction constants b , decreasing values of the nuclear quadrupole moment Q were obtained in 5, 6, 7, and 8 p 2 P 3/2 . When core polarization effects are taken into account, the different 2 P 3/2 levels yield consistent values for the quadrupole moment. We find ----- -- g J (5 p 2 P 3/2 ) = -1.3362 (6) -- g J (6 p 2 P 3/2 ) = -1.3347 (10) ----- -- Ï (5 p 2 P 3/2 ) = 25.8 (8) ns -- Ï (6 p 2 P 3/2 ) = 111 (3) ns ----- -- b (5 p 2 P 3/2 ) = 12.510 (57) MHz -- b (6 p 2 P 3/2 ) = 3.947 (13) MHz ----- -- Q (5 p 2 P 3/2 ) = 0.131 barn -- Q (6 p 2 P 3/2 ) = 0.133 barn ----- -- g J (7 p 2 P 3/2 ) = -1.3359 (11) -- a (8 p 2 P 3/2 ) = 6.747 (14) MHz ----- -- Ï (7 p 2 P 3/2 ) = 233 (10) ns -- b (8 p 2 P 3/2 ) = 0.933 (20) MHz ----- -- b (7 p 2 P 3/2 ) = 1.768 (8) MHz -- Q (8 p 2 P 3/2 ) = 0.131 barn ----- -- Q (7 p 2 P 3/2 ) = 0.133 barn -- ----- Considering possible sources of error in the evaluation of the quadrupole moment we obtain Q (Rb 87 ) = +0.132 (9) barn.}},
author = {{Belin, G and Svanberg, Sune}},
issn = {{0031-8949}},
language = {{eng}},
number = {{6}},
pages = {{269--273}},
publisher = {{IOP Publishing}},
series = {{Physica Scripta}},
title = {{Electronic gJ Factors, Natural Lifetimes, and Electric Quadrupole Interaction for Rb 87 in the np ^(2)P_(3/2) Series of the Rb I Spectrum}},
url = {{https://lup.lub.lu.se/search/files/6372755/2297031.pdf}},
doi = {{10.1088/0031-8949/4/6/006}},
volume = {{4}},
year = {{1971}},
}