Mathematica (v. 11.0.0.0) code for a solution of the 5x5 matrix for optical pumping with circularly polarized (sigma+) light for the D2 transition in Rb-87, Fg=2->Fg=3 line, in the presence of an external magnetic field.
Mathematica (v. 11.0.0.0) code for a solution of the 5x5 matrix for optical pumping with circularly polarized (sigma+) light for the D2 transition in Rb-87, Fg=2->Fg=3 line, in the absence of an external magnetic field.
We present results of a method for calculating optical pumping rates in 87 Rb, as described in [1]. We use circularly polarised light on the (F g = 2 ↔ F e = 3) transition to populate a stretched angular momentum state in the F g = 2 hyperfine structure level of the ground state. The method is shown to function well for the the studied system....
We present results of a method for calculating optical pumping rates in 87 Rb, as described in [1]. We use linearly polarized light on the (F g = 2 ↔ F e = 2) transition to populate an angular momentum state in the F g = 2 hyperfine structure level of the ground state, with magnetic quantum number M g = 0 — that is a clock state. The open decay...
We present results of a method for calculating optical pumping rates in 87 Rb, as described in [1]. We use light with an impure polarization (i.e. a mixture of σ + , σ − and π light) to populate a stretched angular momentum state in the F g = 2 hyperfine structure level of the ground state. The method is shown to function well for the studied...
Mathematica (v. 11.0.0.0) code for a solution of the 5x5 matrix for optical pumping with circularly polarized (sigma+) light for the D2 transition in Rb-87, Fg=2->Fe=3 line, in the absence of an external magnetic field. The light polarization is contaminated by components of (sigma-) and (pi) polarizations. More generally, the code can be used...
We present results of a method for calculating optical pumping rates in 87 Rb, as described in [1]. We use circularly polarized light to populate a stretched angular momentum state in the F g = 2 hyperfine structure level of the ground state. We include in the analysis an applied weak magnetic field. The method is shown to function well for the...
We present results of a method for calculating optical pumping rates in 87 Rb, as described in [1]. We use a mixture of circularly polarised light (σ + and σ −) on the (F g = 1 ↔ F e = 0) transition to populate an angular momentum state in the F g = 1 hyperfine structure level of the ground state, with magnetic quantum number M g = 0 — that is...
Mathematica (v. 11.0.0.0) code for a solution of the 3x3 matrix for optical pumping with mixture of sigma+ and sigma- light for the D2 transition in Rb-87, Fg=1->Fg=0, in the absence of an external magnetic field.
Mathematica (v. 11.0.0.0) code for a solution of the 8x8 matrix for optical pumping with linear polarization for the D2 transition in Rb-87, Fg=2->Fg=2, in the absence of an external magnetic field. In order to avoid optical depumping to Fg=1, repumping light on the transition Fg=1->Fe=2 has been added.