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author | Eugeniy Mikhailov <evgmik@gmail.com> | 2010-01-13 21:04:24 +0000 |
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committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2010-01-13 21:04:24 +0000 |
commit | 566822ec69ba20afe83541546b2fc99b11f3a9c8 (patch) | |
tree | f7192486268e625c14f4baa27e96315661074f90 /liouville.m | |
parent | 97c16478c617405d5c7e8e2e8fc7511fd0904709 (diff) | |
download | multi_mode_eit-566822ec69ba20afe83541546b2fc99b11f3a9c8.tar.gz multi_mode_eit-566822ec69ba20afe83541546b2fc99b11f3a9c8.zip |
typo fix
Diffstat (limited to 'liouville.m')
-rw-r--r-- | liouville.m | 3 |
1 files changed, 2 insertions, 1 deletions
diff --git a/liouville.m b/liouville.m index e37b947..5a54a32 100644 --- a/liouville.m +++ b/liouville.m @@ -60,10 +60,11 @@ E_field_lad.left = E_field_zero + (0.00000+0.00000i)*E_field_probe + (0.00000 % phi is angle between linear polarization and axis x phi=pi*2/8; -% theta is angle between lab z axis (light porpagation dirextion) and magnetic field axis (z') +% theta is angle between lab z axis (light propagation direction) and magnetic field axis (z') theta=pi/2; % we define light as linearly polarized +% where phi is angle between light polarization and axis x E_field_lab.x=cos(phi)*E_field_lab.linear; E_field_lab.y=sin(phi)*E_field_lab.linear; E_field_lab.z=E_field_zero; |