Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...

F’=2 −
F’=1
mF = −2 mF = −1 mF = 0 mF = 1 mF = 2
1
6
−
1
24
1
8
0
1
6
1
24
1
8
Table B.9: Sodium D1-line hyperfine dipole transition matrix elements for π transitions
(F = 2mF → F ′ m ′
F = mF) in multiples of 〈J = 1
2 ||µ2 ||J ′ = 1
2 〉
1
6
mF = −2 mF = −1 mF = 0 mF = 1 mF = 2
F’=2 −
F’=1
1
12
1
8
1
24
−
1
8
1
8
Table B.10: Sodium D1-line hyperfine dipole transition matrix elements for σ− transitions
(F = 2mF → F ′ m ′
F = mF − 1) in multiples of 〈J = 1
2 ||µ2 ||J ′ = 1
2 〉
F’=2 −
F’=1 −
−
mF = −1 mF = 0 mF = 1
1
24
1
24
−
−
1
8
1
24
Table B.11: Sodium D1-line hyperfine dipole transition matrix elements for σ + transitions
(F = 1mF → F ′ m ′
F = mF + 1) in multiples of 〈J = 1
2 ||µ2 ||J ′ = 1
2 〉
F’=2
F’=1
1
2
mF = −1 mF = 0 mF = 1
1
8
1
6
1
24 0 −
1
8
1
24
Table B.12: Sodium D1-line hyperfine dipole transition matrix elements for π transitions
(F = 1mF → F ′ m ′
F = mF) in multiples of 〈J = 1
2 ||µ2 ||J ′ = 1
2 〉
F’=2 − 1
2
F’=1
mF = −1 mF = 0 mF = 1
1
8
1
24
−
1
24
1
24
Table B.13: Sodium D1-line hyperfine dipole transition matrix elements for σ− transitions
(F = 1mF → F ′ m ′
F = mF − 1) in multiples of 〈J = 1
2 ||µ2 ||J ′ = 1
2 〉
61
−
−
1
12
1
2