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-rw-r--r--xmds2/Nlevels_with_doppler_with_z_4wm/Nlevels_with_doppler_with_z_4wm.xmds8
1 files changed, 7 insertions, 1 deletions
diff --git a/xmds2/Nlevels_with_doppler_with_z_4wm/Nlevels_with_doppler_with_z_4wm.xmds b/xmds2/Nlevels_with_doppler_with_z_4wm/Nlevels_with_doppler_with_z_4wm.xmds
index c63870e..d8fd6a4 100644
--- a/xmds2/Nlevels_with_doppler_with_z_4wm/Nlevels_with_doppler_with_z_4wm.xmds
+++ b/xmds2/Nlevels_with_doppler_with_z_4wm/Nlevels_with_doppler_with_z_4wm.xmds
@@ -50,7 +50,8 @@
const double lambda=794.7e-9; //wavelength in m
const double Kvec = 2*M_PI/lambda; // k-vector
const double Gamma_super=6*(2*M_PI*1e6); // characteristic decay rate of upper level used for eta calculations expressed in [1/s]
- const double eta = 3*lambda*lambda*Ndens*Gamma_super/8.0/M_PI; // eta constant in the wave equation for Rabi frequency. Units are [1/(m s)]
+ // eta will be calculated in the sequence -> filter element to use --Ndens parameter
+ double eta = 0; // eta constant in the wave equation for Rabi frequency. Units are [1/(m s)]
// --------- Atom and cell properties -------------------------
// range of Maxwell distribution atomic velocities
@@ -287,6 +288,11 @@
</vector>
<sequence>
+ <filter>
+ <![CDATA[
+ eta = 3*lambda*lambda*Ndens*Gamma_super/8.0/M_PI; // eta constant in the wave equation for Rabi frequency. Units are [1/(m s)]
+ ]]>
+ </filter>
<!--For this set of conditions ARK45 is faster than ARK89-->
<!--ARK45 is good for small detuning when all frequency like term are close to zero-->
<integrate algorithm="ARK45" tolerance="1e-5" interval="Lcell">