nettoyage code

calculation.py

@@ -33,8 +33,6 @@ def refra(bypass_dbr=True, electric_field=0., wavelength=850e-9):
     plt.plot_refra(sl)
 
 
-
-
 def al_doping(bypass_dbr=True):
     sl = st.structure_eam_vcsel(eam_only=True, bypass_dbr=bypass_dbr)
     plt.plot_al_doping(sl)
@@ -73,29 +71,6 @@ def reflectivity(bypass_dbr=True,
         return r
 
 
-def dbr_reflectivity(start_wavelength=700e-9,
-                 stop_wavelength=1000e-9,
-                 electric_field=0.,
-                 n_points=100,
-                 plot=True):
-    wavelength = np.linspace(start_wavelength, stop_wavelength, num=n_points)
-    r = np.zeros(len(wavelength))
-
-    # wavelength in [m]
-    # wavelength must be a numpy array
-    for i in tqdm(range(len(wavelength))):
-        sl = st.structure_dbr(period=20, grading_type = 'linear slope')
-        sl = op.algaas_super_lattice_refractive_index(sl, electric_field, wavelength[i], lengyel=True)
-
-        n = sl['refractive_index'].to_numpy(dtype=np.complex128)
-        d = sl['thickness'].to_numpy(dtype=float)
-
-        r[i] = tmm.reflection(n, d, wavelength[i])
-
-    if plot:
-        plt.plot_reflectivity(wavelength, r)
-    else:
-        return
 
 
 def reflectivity_heatmap(bypass_dbr=True,
@@ -199,16 +174,6 @@ def clad_coupling_electromagnetic_amplitude(bypass_dbr=False, electric_field=0.,
     plt.plot_refra_clad_coupling_em(sl1, sl2, sl3)
 
 
-def animation_clad_coupling(bypass_dbr=False, electric_field=0., wavelength=850e-9):
-    cladding = np.linspace(9.9e-9, 10.1e-9, 9)
-
-    for cl in cladding:
-        sl = st.structure_eam_vcsel(bypass_dbr=bypass_dbr, vcsel_only=True, grading_type='none', mqw_alloy_type='none', l_vcsel_clad=cl)
-        sl = op.algaas_super_lattice_refractive_index(sl, electric_field, wavelength)
-        sl = pt.cut_in_equal_layers_thickness(sl, 5e-9)
-        em = tmm.em_amplitude_scattering_matrix(sl, wavelength)
-        sl.insert(sl.shape[1], 'electromagnetic_amplitude', value=em)
-        plt.plot_refra_em(sl, str(cl))
 
 
 def zandberg_electromagnetic_amplitude(electric_field=0., wavelength=1e-6):
@@ -273,7 +238,7 @@ def ftir_theory_comparison_reflectivity(filename='eam_2', electric_field=0., doc
 
 
 def mqw_psi(lz=0.01e-9):
-    sl = st.structure_eam_vcsel(eam_mqw_only=True, amount_eam_qw=5)
+    sl = st.structure_eam_vcsel(amount_eam_qw=5)
     sl = pt.cut_in_equal_layers_thickness(sl, lz)
     v_e, v_hh, eig_e, psi_e, eig_hh, psi_hh = qt.solve_schrodinger(sl)
     np.savez_compressed('v_e', v_e)

macro.py

@@ -35,6 +35,8 @@ def eam_heatmaps():
                             r_file_name='heatmap_r_eam_2')
 
 
+
+
 def reflectivity_eam_vcsel_clad_heatmap():
     n_pts = 30
     l_eam_clad =np.linspace(15, 20, num=n_pts)
@@ -59,6 +61,8 @@ def reflectivity_eam_vcsel_clad_heatmap():
     plt.plot_std_heatmap(l_eam_clad, l_vcsel_clad, r)
 
 
+
+
 def structure_for_matlab(vcsel_only=False, bypass_dbr=False, wavelength=850.5e-9):
     l_eam_clad = 5e-9
     l_vcsel_clad = 15e-9
@@ -70,5 +74,3 @@ def structure_for_matlab(vcsel_only=False, bypass_dbr=False, wavelength=850.5e-9
     n = sl['refractive_index'].apply(np.real).to_numpy(dtype=float)
 
     scipy.io.savemat('eam_vcsel_n_lz.mat', dict(n=n, lz=lz))
-
-

plan

 OBJECTIFS
-    Nettoyer le code de la structure python.
-
     Traiter les courbes mesurées de la refléctivité temporelle.
     Les comparer aux calculs théoriques.
 
-    Faire l'épitaxie.
     Faire le fit du FTIR.
 
     Vérifier les recettes avec Alexandre
-
-
+    Faire l'épitaxie.
 
 
 ACCOMPLI
+    Nettoyer le code de la structure python.
     Faire les calculs VCSEL EAM avec oxydation eam.
     Réinstaller crystal XE et faire les recettes EAM-VCSELs.
     Corriger le tmm !!!!!!!!!
@@ -20,8 +17,4 @@ ACCOMPLI
 
 ECHOUÉ
     FTIR.
-    Calcul carte de chaleur reflectivité
-
-
-QUESTIONS
-
+    Calcul carte de chaleur reflectivité
\ No newline at end of file