diff options
Diffstat (limited to 'xmds2')
| -rw-r--r-- | xmds2/Nlevels_no_dopler_with_z/Nlevels_no_dopler_with_z.xmds | 69 |
1 files changed, 30 insertions, 39 deletions
diff --git a/xmds2/Nlevels_no_dopler_with_z/Nlevels_no_dopler_with_z.xmds b/xmds2/Nlevels_no_dopler_with_z/Nlevels_no_dopler_with_z.xmds index 718cf76..a210522 100644 --- a/xmds2/Nlevels_no_dopler_with_z/Nlevels_no_dopler_with_z.xmds +++ b/xmds2/Nlevels_no_dopler_with_z/Nlevels_no_dopler_with_z.xmds @@ -29,62 +29,52 @@ * ------- |1> * - We moved to dimensionless units - t -> t*DecayRateNormalization ,time - z -> z*DecayRateNormalization/c , distance - rabi_frequency -> rabi_frequency/DecayRateNormalization - eta -> eta*c/DecayRateNormalization^2 , coupling constant - gij -> gij/DecayRateNormalization - Wij -> Wij/DecayRateNormalization - - where g is 1MHz rate We are solving - dE/dz+(1/c)*dE/dt=i*eta*rho_ij, where j llevel is higher then i + dE/dz+(1/c)*dE/dt=i*eta*rho_ij, where j level is higher then i. + Note that E is actually a Rabi frequency of electromagnetic field not the EM field in xmds terms it looks like - dE_dz = i*eta*rhoij - L[E], here we moved t dependence to Fourier space + dE_dz = i*eta*rhoij - 1/c*L[E], here we moved t dependence to Fourier space + + VERY IMPORTANT: all Rabi frequency should be given in [1/s], if you want to + normalize it to something else look drho/dt equation. + No need to renormalizes eta as long as its express through i + the upper level decay rate in the same units as Rabi frequency. </description> <features> <globals> <![CDATA[ const double pi = M_PI; - const double DecayRateNormalization=10e6; // measured in s^-1 - const double c=3e8; + const double c=3.e8; const double lambda=794.7e-9; //wavelength in m - const double N=1e9; //number of particles per cubic cm - const double eta = 3*lambda*lambda*(N/1e-6)/8.0/pi*c/DecayRateNormalization; //dimensionless coupling constant + const double N=1e10*(1e6); //number of particles per cubic m i.e. density + const double Gamma=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*N*Gamma/8.0/M_PI; // eta constant in the wave equation for Rabi frequency. Units are [1/(m s)] - // repopulation rate (atoms flying in/out the laser beam) in MHz - const double gt=0.01/2; - // Natural linewidth of j's level in MHz - const double G3=2*2.7; - const double G4=2*3.0; + // repopulation rate (atoms flying in/out the laser beam) in [1/s] + const double gt=0.01/2 *(2*M_PI*1e6); + // Natural linewidth of j's level in [1/s] + const double G3=2*2.7 *(2*M_PI*1e6); + const double G4=2*3.0 *(2*M_PI*1e6); - // branching ratios + // total decay of i-th level branching ratios. Rij branching of i-th level to j-th const double R41=0.5, R42=0.5; const double R31=0.5, R32=0.5; - //const double delta1=0; // E2 detuning in MHz - //const double delta2=0; // E2 detuning in MHz - //const double delta3=0; // E3 detuning in MHz - - //const complex E1o=0.005/2; // Rabi frequency in MHz - //const complex E2o=5.0/2; // Rabi frequency in MHz - //const complex E3o=6.0/2; // Rabi frequency in MHz complex E1c, E2c, E3c; // Complex conjugated Rabi frequencies - complex r21, r31, r41, r32, r42, r43, r44; + complex r21, r31, r41, r32, r42, r43, r44; // density matrix elements ]]> </globals> <benchmark /> <arguments> - <!--Rabi frequency divided by 2--> - <argument name="E1o" type="real" default_value="0.0025" /> - <argument name="E2o" type="real" default_value="2.5" /> - <argument name="E3o" type="real" default_value="3.0" /> - <!--Fields detuning in MHz--> + <!-- Rabi frequency divided by 2 in [1/s] --> + <argument name="E1o" type="real" default_value="0.0025*(2*M_PI*1e6)" /> + <argument name="E2o" type="real" default_value="6*(2*M_PI*1e6)" /> + <argument name="E3o" type="real" default_value="0.0*(2*M_PI*1e6)" /> + <!-- Fields detuning in [1/s] --> <argument name="delta1" type="real" default_value="0.0" /> <argument name="delta2" type="real" default_value="0.0" /> <argument name="delta3" type="real" default_value="0.0" /> @@ -95,21 +85,22 @@ <auto_vectorise /> </features> - <!-- Let's convert 'z' and 't' to dimentionless units over here --> + <!-- 'z' and 't' to have dimensions [m] and [s] --> <geometry> <propagation_dimension> z </propagation_dimension> <transverse_dimensions> - <dimension name="t" lattice="1000" domain="(-2.0, 4.0)" /> + <dimension name="t" lattice="1000" domain="(-2.0e-6, 4.0e-6)" /> </transverse_dimensions> </geometry> + <!-- Rabi frequency --> <vector name="E_field" type="complex" initial_space="t"> <components>E1 E2 E3</components> <initialisation> <![CDATA[ // Initial (at starting 'z' position) electromagnetic field does not depend on detuning // as well as time - E1=E1o*exp(-pow( ((t-0.0)/1),2) ); + E1=E1o*exp(-pow( ((t-0.0)/1e-6),2) ); E2=E2o; E3=E3o; ]]> @@ -146,7 +137,7 @@ <sequence> <!--For this set of conditions ARK45 is faster than ARK89--> - <integrate algorithm="ARK45" tolerance="1e-2" interval="4e-2"> + <integrate algorithm="ARK45" tolerance="1e-5" interval="7e-2"> <!--SIC algorithm seems to be much slower and needs fine 'z' step tuning and much finer time grid--> <!--For example I had to quadruple the time grid from 1000 to 4000 when increased z distance from 0.02 to 0.04--> @@ -193,7 +184,7 @@ <operator kind="ex" constant="yes"> <operator_names>Lt</operator_names> <![CDATA[ - Lt = i*kt; + Lt = i*1./c*kt; ]]> </operator> <integration_vectors>E_field</integration_vectors> |