diff --git a/yambopy/bse/excitondipoles.py b/yambopy/bse/excitondipoles.py
index 70d42136..2baf899c 100644
--- a/yambopy/bse/excitondipoles.py
+++ b/yambopy/bse/excitondipoles.py
@@ -135,7 +135,7 @@ def exc_dipoles_pol(lattice_path,dipoles_path=None,bse_path=None,save_files=True
     # Since we have dipoles for emission, we do not conjugate BS_wfc
     # Then the results are directly the exciton dipoles for emission
     dip_exc = np.einsum('nkcv,kicv->in',BS_wfc,dip_expanded,
-                        optimize=True).astype(dtype=dipoles.dtype)
+                        optimize=True).astype(dtype=dipoles.dtype)/np.sqrt(yexc.nkpoints)
 
     if save_files:
         if dip_file[-4:]!='.npy': dip_file = dip_file+'.npy'
diff --git a/yambopy/dbs/excitondb.py b/yambopy/dbs/excitondb.py
index 5045df35..446b065b 100644
--- a/yambopy/dbs/excitondb.py
+++ b/yambopy/dbs/excitondb.py
@@ -336,7 +336,6 @@ def real_wf_to_cube(self, iexe, wfdb, fixed_postion=[0,0,0], supercell=[1,1,1],
         excQpt = self.car_qpoint
         # Convert the q-point to crystal coordinates
         Qpt = wfdb.ydb.lat @ excQpt
-        print("Qpt: ",Qpt)
         #
         if fix_particle == 'h': name_file = 'electron'
         else: name_file = 'hole'